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      "may_be_used_as_earlier_proved_premise": false,
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          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
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          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
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      "scope_boundary": "Exact positive-label notation; context, not a separate proved result"
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      "source_level_hypothesis_ranges": [
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          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
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      "scope_boundary": "Compact-plus-closed sums and exact two-step spectral sandwich bound"
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      "source_level_hypothesis_ranges": [
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          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
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      "scope_boundary": "Arbitrary family range detection in both corner orientations"
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    {
      "id": "OA-FLOW.L121.SC2",
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          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
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      "source_level_hypothesis_ranges": [
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          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
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          "full_statement_context": "Assume now \\(Z(M)^\\alpha=\\mathbb C1\\). We construct a family satisfying SC2 for any prescribed nonzero central fixed corners and any identity neighborhood. The retained equations (D2)–(D23) make every step explicit.\n",
          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
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          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
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        "OA-FLOW.CP.6",
        "OA-FLOW.XGAPS.CSTAR.H0",
        "OA-FLOW.L115.CONVENTIONS"
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      "source_level_hypothesis_ranges": [
        {
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          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
        },
        {
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          "full_statement_context": "Assume now \\(Z(M)^\\alpha=\\mathbb C1\\). We construct a family satisfying SC2 for any prescribed nonzero central fixed corners and any identity neighborhood. The retained equations (D2)–(D23) make every step explicit.\n",
          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
        },
        {
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          "full_statement_context": "Throughout, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\) has its additive dual-group law, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary Hilbert space \\(\\mathcal H\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is a point-ultraweakly continuous action by normal automorphisms. Put \\(F=M^\\alpha\\). No separability, countability, sigma-finiteness or factor hypothesis is assumed. SC0–SC2 require no central ergodicity; SC3–SC4 additionally assume \\(Z(M)^\\alpha=\\mathbb C1\\), exactly where stated.\n",
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          "full_statement_context": "Assume now \\(Z(M)^\\alpha=\\mathbb C1\\). We construct a family satisfying SC2 for any prescribed nonzero central fixed corners and any identity neighborhood. The retained equations (D2)–(D23) make every step explicit.\n",
          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
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          "usage": "Exact source-level context applies subject to the local statement. Context is not an earlier proved premise."
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        "OA-FLOW.CP.6"
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          "source": "src/OA-FLOW-L122.md",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
          "usage": "Full global setting and frequency convention, subject to explicit local hypotheses; context is not a proof premise."
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          "usage": "Full global setting and frequency convention, subject to explicit local hypotheses; context is not a proof premise."
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          "full_statement_context": "<a id=\"ia-setting\"></a>\n# Small fixed corners, inner spectra and annihilating times\n\nA globally fixed unitary can implement an action at a time only if every Connes frequency evaluates to one there. The mechanism is a nonzero fixed corner on which conjugation is arbitrarily close to the identity in operator norm. We construct that corner first, so this application does not depend on the later product-spectrum theorem. We then prove the universal quotient bound and explain exactly how a factor supplies the missing lower bound.\n\nThroughout, \\(M\\ne0\\) is a von Neumann algebra on an arbitrary complex Hilbert space \\(\\mathcal H\\), and \\(u\\in\\mathcal U(M)\\). For the action statements, \\(G\\) is an arbitrary locally compact Hausdorff abelian group, \\(H=\\widehat G\\), and \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) is point-ultraweakly continuous with normal unital star automorphisms. Write \\(N=M^\\alpha\\). There is no separability, sigma-finiteness, countability, finite-Haar, central-ergodicity or factor hypothesis unless it is explicitly introduced.\n\nThe ordinary complex spectrum in the algebra \\(M\\), or in the Banach algebra of bounded operators on \\(M\\), will be denoted by \\(\\sigma\\) or \\(\\operatorname{Sp}\\) with the algebra shown. The action spectrum is a closed subset of \\(H\\). These are different objects. The positive frequency convention is the exact earlier [L115 convention](OA-FLOW-L115.md#oa-flow.l115.conventions): \\(p(s)=(s,p)\\). The earlier GCC negative-label spectrum reflects vector labels, but adjoint reflection makes each whole corner action spectrum symmetric. Its positive and negative versions, and their Connes intersections, consequently agree. No individual vector spectrum is assumed symmetric.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l122.inputs\"></a>\n\n<a id=\"ia-inputs\"></a>\n## Exact earlier proof inputs\n\nThe eleven direct earlier scopes are [CF1](OA-FLOW-CF.md#oa-flow.cf.1) (choice and maximality), [CF2](OA-FLOW-CF.md#oa-flow.cf.2) (Banach spectrum and geometric series), [CF4](OA-FLOW-CF.md#oa-flow.cf.4) (characters), [CF6](OA-FLOW-CF.md#oa-flow.cf.6) (isometric continuous calculus and automorphism contractivity), [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1) (corners, supports and polar decomposition), [PC2](OA-FLOW-PC.md#oa-flow.projection.pc2) (central support and nonzero bridges), [GCC SETTING](OA-FLOW-GCC.md#gcc-setting), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [GCC DEFINITION](OA-FLOW-GCC.md#gcc-definition), [L115 CONVENTIONS](OA-FLOW-L115.md#oa-flow.l115.conventions), and [OPSP FORMULA](OA-FLOW-L89.md#oa-flow.opsp.formula).\n\nFor OPSP the scope includes its full source setting and proof O1–O9, the actual [AF0](OA-FLOW-AF.md#af-0) specified-dual hypotheses, and the full [AT1–3](OA-FLOW-AT.md#oa-flow.at.3) bridge. Those contexts are necessary: mere ultraweak continuity must be connected to norm continuity of every orbit in the actual predual. They are complete inherited contexts within the eleven-root closure, not extra direct proof roots. Opening descriptions, source comparisons and illustrations are never proof providers.\n\n",
          "usage": "Full global setting and frequency convention, subject to explicit local hypotheses; context is not a proof premise."
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          "usage": "Full global setting and frequency convention, subject to explicit local hypotheses; context is not a proof premise."
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      "scope_boundary": "Bounded source comparison and retained history; never a mathematical proof provider"
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.historical.setting\"></a><a id=\"l123-historical-setting\"></a>\n## Maximal-remainder proof: tensor-product innerness from slice intertwiners\n\nIf a tensor product of two automorphisms is inner, each factor automorphism is inner.  The reverse implication is immediate; the content is extracting a nonzero intertwiner from an implementing tensor unitary, turning its polar part into a unitary on an invariant central summand, and patching all such summands without a countability assumption.\n\nLet $M_1,M_2$ be nonzero von Neumann algebras, let $\\sigma_i\\in\\operatorname{Aut}(M_i)$, and put\n\n<a id=\"equation-t1\"></a>\n$$\nM=M_1\\,\\overline\\otimes\\,M_2,\n\\qquad\n\\sigma=\\sigma_1\\,\\overline\\otimes\\,\\sigma_2.\n\\tag{T1}\n$$\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.historical.setting\"></a><a id=\"l123-historical-setting\"></a>\n## Maximal-remainder proof: tensor-product innerness from slice intertwiners\n\nIf a tensor product of two automorphisms is inner, each factor automorphism is inner.  The reverse implication is immediate; the content is extracting a nonzero intertwiner from an implementing tensor unitary, turning its polar part into a unitary on an invariant central summand, and patching all such summands without a countability assumption.\n\nLet $M_1,M_2$ be nonzero von Neumann algebras, let $\\sigma_i\\in\\operatorname{Aut}(M_i)$, and put\n\n<a id=\"equation-t1\"></a>\n$$\nM=M_1\\,\\overline\\otimes\\,M_2,\n\\qquad\n\\sigma=\\sigma_1\\,\\overline\\otimes\\,\\sigma_2.\n\\tag{T1}\n$$\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.historical.setting\"></a><a id=\"l123-historical-setting\"></a>\n## Maximal-remainder proof: tensor-product innerness from slice intertwiners\n\nIf a tensor product of two automorphisms is inner, each factor automorphism is inner.  The reverse implication is immediate; the content is extracting a nonzero intertwiner from an implementing tensor unitary, turning its polar part into a unitary on an invariant central summand, and patching all such summands without a countability assumption.\n\nLet $M_1,M_2$ be nonzero von Neumann algebras, let $\\sigma_i\\in\\operatorname{Aut}(M_i)$, and put\n\n<a id=\"equation-t1\"></a>\n$$\nM=M_1\\,\\overline\\otimes\\,M_2,\n\\qquad\n\\sigma=\\sigma_1\\,\\overline\\otimes\\,\\sigma_2.\n\\tag{T1}\n$$\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.historical.setting\"></a><a id=\"l123-historical-setting\"></a>\n## Maximal-remainder proof: tensor-product innerness from slice intertwiners\n\nIf a tensor product of two automorphisms is inner, each factor automorphism is inner.  The reverse implication is immediate; the content is extracting a nonzero intertwiner from an implementing tensor unitary, turning its polar part into a unitary on an invariant central summand, and patching all such summands without a countability assumption.\n\nLet $M_1,M_2$ be nonzero von Neumann algebras, let $\\sigma_i\\in\\operatorname{Aut}(M_i)$, and put\n\n<a id=\"equation-t1\"></a>\n$$\nM=M_1\\,\\overline\\otimes\\,M_2,\n\\qquad\n\\sigma=\\sigma_1\\,\\overline\\otimes\\,\\sigma_2.\n\\tag{T1}\n$$\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.historical.setting\"></a><a id=\"l123-historical-setting\"></a>\n## Maximal-remainder proof: tensor-product innerness from slice intertwiners\n\nIf a tensor product of two automorphisms is inner, each factor automorphism is inner.  The reverse implication is immediate; the content is extracting a nonzero intertwiner from an implementing tensor unitary, turning its polar part into a unitary on an invariant central summand, and patching all such summands without a countability assumption.\n\nLet $M_1,M_2$ be nonzero von Neumann algebras, let $\\sigma_i\\in\\operatorname{Aut}(M_i)$, and put\n\n<a id=\"equation-t1\"></a>\n$$\nM=M_1\\,\\overline\\otimes\\,M_2,\n\\qquad\n\\sigma=\\sigma_1\\,\\overline\\otimes\\,\\sigma_2.\n\\tag{T1}\n$$\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.historical.setting\"></a><a id=\"l123-historical-setting\"></a>\n## Maximal-remainder proof: tensor-product innerness from slice intertwiners\n\nIf a tensor product of two automorphisms is inner, each factor automorphism is inner.  The reverse implication is immediate; the content is extracting a nonzero intertwiner from an implementing tensor unitary, turning its polar part into a unitary on an invariant central summand, and patching all such summands without a countability assumption.\n\nLet $M_1,M_2$ be nonzero von Neumann algebras, let $\\sigma_i\\in\\operatorname{Aut}(M_i)$, and put\n\n<a id=\"equation-t1\"></a>\n$$\nM=M_1\\,\\overline\\otimes\\,M_2,\n\\qquad\n\\sigma=\\sigma_1\\,\\overline\\otimes\\,\\sigma_2.\n\\tag{T1}\n$$\n\n",
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          "full_statement_context": "<a id=\"oa-flow.l123.setting\"></a><a id=\"l123-setting\"></a>\n# From an intertwiner family to tensor-product innerness\n\nA single normal state can send a tensor unitary to zero. A family of separating states keeps the information we need: its slice intertwiners have central carriers whose join is the identity. We first construct the actual tensor product and normal maps, then show how any family of intertwiners assembles a largest inner central part. Constructed normal slices will supply a family with full support. The maximal-remainder argument gives a second complete proof.\n\nThroughout, \\(M_i\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space \\(H_i\\), with identity \\(1_{H_i}\\), and \\(\\sigma_i\\) is an algebraic unital star automorphism of \\(M_i\\). Thus \\(H_i\\ne0\\). For the single-algebra statements, \\(N\\ne0\\) is a concrete von Neumann algebra on an arbitrary Hilbert space \\(K\\), with automorphism \\(\\sigma\\). Inner products are linear in the first variable. An automorphism is inner if it has the form \\(x\\mapsto v x v^*\\) for a unitary \\(v\\) in the actual algebra. A central corner \\(zN\\) has identity \\(z\\); its implementing unitary satisfies \\(v^*v=vv^*=z\\). There is no factor, separability, countability, sigma-finiteness or faithful-normal-state assumption. Arbitrary orthogonal sums below mean nets over finite subsets.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n## Exact earlier inputs\n\nThe thirteen direct proofs are [CF1](OA-FLOW-CF.md#oa-flow.cf.1), [CF6](OA-FLOW-CF.md#oa-flow.cf.6), [CF8](OA-FLOW-CF.md#oa-flow.cf.8), [CP1](OA-FLOW-CP.md#oa-flow.cp.1), [CP2](OA-FLOW-CP.md#oa-flow.cp.2), [CP4](OA-FLOW-CP.md#oa-flow.cp.4), [CP6](OA-FLOW-CP.md#oa-flow.cp.6), [PC1](OA-FLOW-PC.md#oa-flow.pc.1), [GCC TOOLS](OA-FLOW-GCC.md#gcc-tools), [NCF1](OA-FLOW-NCF.md#ncf-1), [BD4](OA-FLOW-BD.md#oa-flow.bd.4), [BD5](OA-FLOW-BD.md#oa-flow.bd.5), and [NF4](OA-FLOW-NF.md#oa-flow.nf.4).\n\nNF4 concerns a bounded positive functional preserving bounded increasing positive suprema on an arbitrary concrete von Neumann algebra; its full source setting is included. BD4 applies to the actual nondegenerate elementary tensor algebra, and BD5 turns uniformly bounded strong nets into ultraweak nets. NCF1's matrix argument is for an arbitrary auxiliary Hilbert space and a normal homomorphism with the actual concrete preduals; no group theorem from its surrounding lesson is a tensor-map premise. CP2 supplies the algebraic quotient by bilinearity. Its projective norm is not the Hilbert tensor norm: we construct the latter next. The general commutation and support arguments in GCC TOOLS are used at their stated bounded-operator scope, without a group action assumption.\n\n",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "full_statement_context": "Let \\(D\\) now be any von Neumann algebra and let \\(\\delta:\\mathbb T\\to\\operatorname{Aut}(D)\\) be point-ultraweakly continuous. For \\(x\\in D\\), define the Fourier mean by its evaluations:\n",
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          "full_statement_context": "Assume \\(D\\ne0\\) is abelian. Let \\(\\mathcal B\\) be any group of automorphisms commuting with \\(\\delta\\), with \\(D^{\\mathcal B}=\\mathbb C1\\). No topology on \\(\\mathcal B\\) is required. A normal element \\(x\\) in an abelian algebra has equal initial and range supports by PC1; write this common projection \\(s(x)\\). It is the least projection \\(p\\) with \\(px=x\\). An automorphism sends such least projections to such least projections, and multiplication by a nonzero scalar preserves the support. Consequently \\(s(x)\\) is fixed by \\(\\delta\\) whenever \\(x\\in D_n\\). Set\n",
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          "full_statement_context": "Now suppose \\(\\delta\\) is faithful. \\(S=\\{0\\}\\) would make all Fourier means fixed, and CE0 would make the whole action trivial on the nonzero algebra. Otherwise choose the least positive \\(k\\in S\\); division with remainder proves \\(S=k\\mathbb Z\\). If \\(k>1\\), \\(\\delta_{2\\pi/k}\\) fixes every \\(D_n\\); normality and CE0 make it the identity on \\(D\\), contradicting faithfulness. We have proved\n",
          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
        }
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          "full_statement_context": "Let \\(D\\) now be any von Neumann algebra and let \\(\\delta:\\mathbb T\\to\\operatorname{Aut}(D)\\) be point-ultraweakly continuous. For \\(x\\in D\\), define the Fourier mean by its evaluations:\n",
          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
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          "full_statement_context": "Assume \\(D\\ne0\\) is abelian. Let \\(\\mathcal B\\) be any group of automorphisms commuting with \\(\\delta\\), with \\(D^{\\mathcal B}=\\mathbb C1\\). No topology on \\(\\mathcal B\\) is required. A normal element \\(x\\) in an abelian algebra has equal initial and range supports by PC1; write this common projection \\(s(x)\\). It is the least projection \\(p\\) with \\(px=x\\). An automorphism sends such least projections to such least projections, and multiplication by a nonzero scalar preserves the support. Consequently \\(s(x)\\) is fixed by \\(\\delta\\) whenever \\(x\\in D_n\\). Set\n",
          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
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          "full_statement_context": "For a fixed \\(n\\) with \\(c_n=1\\), consider families of nonzero \\(x_i\\in D_n\\) with pairwise orthogonal supports \\(p_i\\). Chain unions remain families, so CF1 gives a maximal family. Each \\(p_i\\) is fixed by \\(\\delta\\); normality, or the order-isomorphism property, fixes their join \\(p\\) and \\(q=1-p\\). If \\(q\\ne0\\), the support join \\(c_n=1\\) yields \\(qx\\ne0\\) for some \\(x\\in D_n\\). Its support lies below \\(q\\), so it extends the family, a contradiction. Hence \\(\\bigvee_i p_i=1\\).\n",
          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
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          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
        }
      ],
      "scope_boundary": "Direct matrix extraction w=a tensor U* and sigma=Ad(a*) on the entire original algebra"
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      "id": "OA-FLOW.L124.CE4",
      "unit": "OA-FLOW-L124",
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        "OA-FLOW.CONNES.CENTERKERNEL",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
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          "full_statement_context": "Throughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n",
          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
        },
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          "source_sha256": "846e413bee8b84cc00c2b6cbcebdf71f62ae5696d9324c59e520e2029b0908bd",
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          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
        }
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      "unit": "OA-FLOW-L124",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
        },
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          "usage": "Full arbitrary-algebra global setting, subject to explicit local hypotheses; context is not a proof premise."
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "<a id=\"l124-historical-setting\"></a>\n<a id=\"oa-flow.l124.historical.setting\"></a>\n## Stabilization and tensor-descent argument\n\nCE0–CE5 provide the Fourier, normality, matrix and arbitrary-family facts used below. The concluding tensor descent uses [From an intertwiner family to tensor-product innerness](OA-FLOW-L123.md#oa-flow.l123.ic4); CE3 also gives a direct matrix-coefficient descent.\n\n## Trivial Connes spectrum and centralizer ergodicity force innerness\n\nTrivial Connes spectrum does not by itself make an automorphism inner.  The missing rigidity comes from the automorphisms commuting with it: if that centralizer acts ergodically on the center, stabilization turns the problem into a faithful circle action on an abelian center.  Its degree-one spectral space contains a unitary, and that unitary implements the stabilized automorphism.\n\nLet $M$ be a nonzero von Neumann algebra and $\\sigma\\in\\operatorname{Aut}(M)$.  Regard $\\sigma$ as the action $n\\mapsto\\sigma^n$ of $\\mathbb Z$, whose dual is written multiplicatively as $\\mathbb T$.  Put\n\n<a id=\"equation-e1\"></a>\n\n$$\n\\operatorname{Aut}_\\sigma(M)\n=\\{\\beta\\in\\operatorname{Aut}(M):\\beta\\sigma=\\sigma\\beta\\}.\n\\tag{E1}\n$$\n\nAssume\n\n<a id=\"equation-e2\"></a>\n\n$$\n\\Gamma(\\sigma)=\\{1\\},\n\\qquad\nZ(M)^{\\operatorname{Aut}_\\sigma(M)}=\\mathbb C1.\n\\tag{E2}\n$$\n\nThere is no separability, sigma-finiteness, or countability hypothesis.\n\n",
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          "full_statement_context": "# Read an inner implementer from a circle eigenunitary\n\nTrivial Connes spectrum acquires force when the commuting automorphisms are ergodic on the center. The mechanism has two parts: a faithful circle action on an abelian algebra admits a unitary of degree one, and a central degree-one unitary in the cyclic stabilization has a matrix coefficient that implements the original automorphism. We prove the circle statement first and construct the matrix descent before applying the Connes-spectrum hypothesis.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"oa-flow.l124.setting\"></a>\n<a id=\"l124-inputs\"></a>\n## The setting and earlier proof bodies\n\nThroughout, \\(M\\ne0\\) is an arbitrary concrete von Neumann algebra on an arbitrary Hilbert space, and \\(\\sigma\\) is a star automorphism of \\(M\\). The cyclic action is \\(j\\mapsto\\sigma^j\\), with discrete group \\(\\mathbb Z\\) and multiplicative dual \\(\\mathbb T\\); its Connes spectrum is the intersection of the spectra of all nonzero fixed corners at the exact [L115 conventions](OA-FLOW-L115.md#oa-flow.l115.conventions). We will prove algebraic automorphisms normal. Circle parameters are modulo \\(2\\pi\\), and circle integrals use \\(d\\theta/(2\\pi)\\).\n\nOur complete earlier inputs are the scalar circle measure and Fejér estimates of [CC0](OA-FLOW-CC.md#oa-flow.cc.0), the summable vector-series and predual-duality proofs [CP4](OA-FLOW-CP.md#oa-flow.cp.4) and [CP6](OA-FLOW-CP.md#oa-flow.cp.6), the maximal principle [CF1](OA-FLOW-CF.md#oa-flow.cf.1), the arbitrary projection joins, bounded polar decomposition and orthogonal sums [PC1](OA-FLOW-PC.md#oa-flow.projection.pc1), the bounded positive functional theorem [NF4](OA-FLOW-NF.md#oa-flow.nf.4), the entire normal amplification and matrix-entry proof [NCF1](OA-FLOW-NCF.md#ncf-1), and L115's complete [stabilization](OA-FLOW-L115.md#oa-flow.connes.stabilization) and [dual-center kernel](OA-FLOW-L115.md#oa-flow.connes.centerkernel) bodies.\n\nOnly CC0's scalar measure and finite polynomial estimates are used; its modular-weight setting is not a hypothesis here. PC1's bounded polar and arbitrary-sum proof is used without the countable-decomposability hypothesis of its later classification sections. NF4 proves a theorem about functionals; the next paragraph supplies the passage to automorphisms. The tensor-descent alternative uses the earlier L123 proof.\n\n",
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
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          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "Begin with any increasing positive net \\(0\\leq x_i\\leq C1\\) in \\(M\\). For \\(j\\geq i\\), the positive difference is between zero and \\(C1\\). Continuous calculus gives \\((x_j-x_i)^2\\leq C(x_j-x_i)\\), hence\n\n<a id=\"equation-co1\"></a>\n\n\\[\n\\|(x_j-x_i)\\xi\\|^2\\leq C\\langle(x_j-x_i)\\xi,\\xi\\rangle.\n\\tag{CO1}\n\\]\n\nFor each \\(\\xi\\), the quadratic values have a finite scalar supremum. Once they are close to it, comparison with a common upper index makes both vector differences small by CO1 and the triangle inequality. Thus \\(x_i\\xi\\) is a Cauchy net. To obtain a limit from Hilbert completeness, choose increasing indices after which its errors are below \\(2^{-n}\\); their sequence converges, and the same errors make the entire net converge to that limit. The vector limits define a linear bounded positive operator of norm at most \\(C\\). Strong convergence puts it in the weakly closed algebra \\(M\\). Passing each quadratic order inequality to the limit shows that this operator dominates the net and is below every selfadjoint upper bound. It is its supremum. Adding a scalar reduces uniformly bounded increasing selfadjoint nets to this case.\n\nIn an abelian von Neumann algebra \\(D\\), commuting selfadjoint elements have the pointwise maximum\n\n<a id=\"equation-co2\"></a>\n\n\\[\na\\vee b=\\tfrac12(a+b+|a-b|).\n\\tag{CO2}\n\\]\n\nCF6 identifies the commutative algebra generated by \\(a,b\\) with continuous scalar functions. If another selfadjoint element of \\(D\\) bounds both, it commutes with them and the same scalar comparison in the enlarged commutative algebra makes it bound their displayed maximum. This is a least upper bound in \\(D\\), not a lattice assertion for noncommuting operators.\n\nFor any uniformly bounded selfadjoint family in \\(D\\), finite maxima form a uniformly bounded increasing net. The preceding limit constructs its supremum in \\(D\\). Addition of a fixed selfadjoint element translates all upper bounds, so commutes with this supremum. A star automorphism is an order isomorphism; applying it and its inverse to the defining upper-bound inequalities proves that it carries a supremum to the supremum of the image family. This particular assertion uses order, without a continuity assumption on the map. Infima follow by changing signs.\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "Begin with any increasing positive net \\(0\\leq x_i\\leq C1\\) in \\(M\\). For \\(j\\geq i\\), the positive difference is between zero and \\(C1\\). Continuous calculus gives \\((x_j-x_i)^2\\leq C(x_j-x_i)\\), hence\n\n<a id=\"equation-co1\"></a>\n\n\\[\n\\|(x_j-x_i)\\xi\\|^2\\leq C\\langle(x_j-x_i)\\xi,\\xi\\rangle.\n\\tag{CO1}\n\\]\n\nFor each \\(\\xi\\), the quadratic values have a finite scalar supremum. Once they are close to it, comparison with a common upper index makes both vector differences small by CO1 and the triangle inequality. Thus \\(x_i\\xi\\) is a Cauchy net. To obtain a limit from Hilbert completeness, choose increasing indices after which its errors are below \\(2^{-n}\\); their sequence converges, and the same errors make the entire net converge to that limit. The vector limits define a linear bounded positive operator of norm at most \\(C\\). Strong convergence puts it in the weakly closed algebra \\(M\\). Passing each quadratic order inequality to the limit shows that this operator dominates the net and is below every selfadjoint upper bound. It is its supremum. Adding a scalar reduces uniformly bounded increasing selfadjoint nets to this case.\n\nIn an abelian von Neumann algebra \\(D\\), commuting selfadjoint elements have the pointwise maximum\n\n<a id=\"equation-co2\"></a>\n\n\\[\na\\vee b=\\tfrac12(a+b+|a-b|).\n\\tag{CO2}\n\\]\n\nCF6 identifies the commutative algebra generated by \\(a,b\\) with continuous scalar functions. If another selfadjoint element of \\(D\\) bounds both, it commutes with them and the same scalar comparison in the enlarged commutative algebra makes it bound their displayed maximum. This is a least upper bound in \\(D\\), not a lattice assertion for noncommuting operators.\n\nFor any uniformly bounded selfadjoint family in \\(D\\), finite maxima form a uniformly bounded increasing net. The preceding limit constructs its supremum in \\(D\\). Addition of a fixed selfadjoint element translates all upper bounds, so commutes with this supremum. A star automorphism is an order isomorphism; applying it and its inverse to the defining upper-bound inequalities proves that it carries a supremum to the supremum of the image family. This particular assertion uses order, without a continuity assumption on the map. Infima follow by changing signs.\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "<a id=\"co1\"></a>\n<a id=\"oa-flow.l125.co1\"></a>\n## CO1. Solve a central bounded cocycle for any group\n\nLet \\(G\\) be any group, let \\(\\alpha\\) be an automorphism action, and let the uniformly bounded family \\(h_s\\in Z(M)_{\\rm sa}\\) satisfy\n\n<a id=\"equation-co3\"></a>\n\n\\[\nh_{st}=h_s+\\alpha_s(h_t).\n\\tag{CO3}\n\\]\n\nPutting \\(s=t=e\\) gives \\(h_e=0\\). Its bounded central transfer is\n\n",
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          "full_conditions_and_proof": "<a id=\"co1\"></a>\n<a id=\"oa-flow.l125.co1\"></a>\n## CO1. Solve a central bounded cocycle for any group\n\nLet \\(G\\) be any group, let \\(\\alpha\\) be an automorphism action, and let the uniformly bounded family \\(h_s\\in Z(M)_{\\rm sa}\\) satisfy\n\n<a id=\"equation-co3\"></a>\n\n\\[\nh_{st}=h_s+\\alpha_s(h_t).\n\\tag{CO3}\n\\]\n\nPutting \\(s=t=e\\) gives \\(h_e=0\\). Its bounded central transfer is\n\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "Throughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n"
        },
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          "full_statement_context": "<a id=\"co2\"></a>\n<a id=\"oa-flow.l125.co2\"></a>\n## CO2. Correct the logarithm without increasing its norm\n\nSuppose \\(v\\) implements an automorphism \\(\\sigma\\) commuting with every \\(\\alpha_s\\), and suppose its principal argument is\n\n<a id=\"equation-co6\"></a>\n\n\\[\nv=e^{ib},\\qquad b=b^*,\\qquad B:=\\|b\\|<\\pi/2.\n\\tag{CO6}\n\\]\n\nThe equality \\(\\operatorname{Ad}(\\alpha_s(v))=\\operatorname{Ad}(v)\\) implies \\(a_s=v^*\\alpha_s(v)\\in\\mathcal U(Z(M))\\): multiply the equality of conjugations on the left by \\(v^*\\) and on the right by \\(\\alpha_s(v)\\) to get \\(a_sx=xa_s\\). Conversely a central unitary quotient makes the conjugations equal.\n\nNow \\(\\alpha_s(v)=va_s\\) commutes with \\(v\\). Their principal arguments commute because continuous calculus commutes with every commuting normal generator. A star automorphism is isometric, by CF6's contractivity applied also to its inverse, and transports continuous calculus by polynomial approximation and uniqueness. Therefore \\(\\alpha_s(b)\\) is the principal argument of \\(\\alpha_s(v)\\). Set\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"co2\"></a>\n<a id=\"oa-flow.l125.co2\"></a>\n## CO2. Correct the logarithm without increasing its norm\n\nSuppose \\(v\\) implements an automorphism \\(\\sigma\\) commuting with every \\(\\alpha_s\\), and suppose its principal argument is\n\n<a id=\"equation-co6\"></a>\n\n\\[\nv=e^{ib},\\qquad b=b^*,\\qquad B:=\\|b\\|<\\pi/2.\n\\tag{CO6}\n\\]\n\nThe equality \\(\\operatorname{Ad}(\\alpha_s(v))=\\operatorname{Ad}(v)\\) implies \\(a_s=v^*\\alpha_s(v)\\in\\mathcal U(Z(M))\\): multiply the equality of conjugations on the left by \\(v^*\\) and on the right by \\(\\alpha_s(v)\\) to get \\(a_sx=xa_s\\). Conversely a central unitary quotient makes the conjugations equal.\n\nNow \\(\\alpha_s(v)=va_s\\) commutes with \\(v\\). Their principal arguments commute because continuous calculus commutes with every commuting normal generator. A star automorphism is isometric, by CF6's contractivity applied also to its inverse, and transports continuous calculus by polynomial approximation and uniqueness. Therefore \\(\\alpha_s(b)\\) is the principal argument of \\(\\alpha_s(v)\\). Set\n\n"
        }
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      "scope_boundary": "Principal-log branch, central additive difference and fixed implementer preserving the original B<pi/2 bound"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "Throughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "Throughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n"
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          "full_statement_context": "Let \\(v\\in\\mathcal U(M)\\) and write \\(P(E)=1_E(v)\\) for a Borel subset of \\(\\mathbb T\\). SB3 constructs these projections on arbitrary Hilbert spaces and proves their uniqueness. Each unitary in \\(M'\\) fixes the continuous calculus and therefore the unique Borel calculus; SF0 puts \\(P(E)\\) in \\(M\\). If \\(E\\) is contained in an angular \\(r\\)-arc about \\(e^{i\\theta}\\), the squared-integral identity SB12 and \\(|e^{it}-1|\\leq|t|\\) give\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "Let \\(v\\in\\mathcal U(M)\\) and write \\(P(E)=1_E(v)\\) for a Borel subset of \\(\\mathbb T\\). SB3 constructs these projections on arbitrary Hilbert spaces and proves their uniqueness. Each unitary in \\(M'\\) fixes the continuous calculus and therefore the unique Borel calculus; SF0 puts \\(P(E)\\) in \\(M\\). If \\(E\\) is contained in an angular \\(r\\)-arc about \\(e^{i\\theta}\\), the squared-integral identity SB12 and \\(|e^{it}-1|\\leq|t|\\) give\n"
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          "full_statement_context": "The compact-set form requires a uniform choice. For nonempty compact \\(E,F\\) with \\(EF^{-1}\\cap\\operatorname{Sp}(S)=\\varnothing\\), inverse continuity from CF2 and compactness from CF1 give\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "The compact-set form requires a uniform choice. For nonempty compact \\(E,F\\) with \\(EF^{-1}\\cap\\operatorname{Sp}(S)=\\varnothing\\), inverse continuity from CF2 and compactness from CF1 give\n"
        }
      ],
      "scope_boundary": "All unitary Borel projections in M, resolvent phase separation and complete uniform compact-set subdivision"
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        "OA-FLOW.CF.6",
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "Throughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n"
        },
        {
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          "full_statement_context": "<a id=\"co4\"></a>\n<a id=\"oa-flow.l125.co4\"></a>\n## CO4. Localize centrally, then apply the order correction\n\nAssume \\(\\operatorname{Sp}(S)\\subset V(\\varepsilon)\\), with \\(0<\\varepsilon<\\pi/2\\). Choose \\(0<\\delta<\\varepsilon\\), so \\(\\delta+\\varepsilon<\\pi\\). Let \\(E\\) be the closed \\(\\delta\\)-arc about \\(e^{i\\theta}\\), and \\(c=z(P(E))\\). For \\(\\eta>0\\), put\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"co4\"></a>\n<a id=\"oa-flow.l125.co4\"></a>\n## CO4. Localize centrally, then apply the order correction\n\nAssume \\(\\operatorname{Sp}(S)\\subset V(\\varepsilon)\\), with \\(0<\\varepsilon<\\pi/2\\). Choose \\(0<\\delta<\\varepsilon\\), so \\(\\delta+\\varepsilon<\\pi\\). Let \\(E\\) be the closed \\(\\delta\\)-arc about \\(e^{i\\theta}\\), and \\(c=z(P(E))\\). For \\(\\eta>0\\), put\n\n"
        },
        {
          "source": "src/OA-FLOW-L125.md",
          "source_sha256": "ea3555a84d4f6a4da38273a48ea29131bd91218bcbe54d012197794b4e896fdb",
          "start_line": 235,
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          "range_sha256": "34cc4a4ca0401e0fbe1b61c5745bfa5d27896b370101d24bcceed4c299ca4fda",
          "full_statement_context": "If \\(0<\\varepsilon<\\pi/4\\), its principal argument \\(b\\) is defined by continuous calculus on that closed arc and has \\(B=\\|b\\|\\leq\\delta+\\varepsilon<2\\varepsilon<\\pi/2\\). CO2 applies to any group action commuting with \\(S\\) and produces\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "If \\(0<\\varepsilon<\\pi/4\\), its principal argument \\(b\\) is defined by continuous calculus on that closed arc and has \\(B=\\|b\\|\\leq\\delta+\\varepsilon<2\\varepsilon<\\pi/2\\). CO2 applies to any group action commuting with \\(S\\) and produces\n"
        }
      ],
      "scope_boundary": "Delta+epsilon corner bound, finite disjoint central partition, actual corner inverses and arbitrary-group fixed implementer with spectrum in V(2epsilon)"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
        },
        {
          "referenced_equation_anchor": "equation-co3",
          "context_role": "additive_cocycle_identity_only_without_CO1_central_selfadjoint_hypotheses",
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          "source": "src/OA-FLOW-L125.md",
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          "full_statement_context": "<a id=\"equation-co3\"></a>\n\n\\[\nh_{st}=h_s+\\alpha_s(h_t).\n\\tag{CO3}\n\\]\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"equation-co3\"></a>\n\n\\[\nh_{st}=h_s+\\alpha_s(h_t).\n\\tag{CO3}\n\\]\n"
        }
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          "full_statement_context": "Throughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "Throughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n"
        },
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          "range_sha256": "99ad243b8bf8414ec6ae89d869dc5b68ef083c9e5d72af3582470ef227e60735",
          "full_statement_context": "Here \\(G\\) is abelian, \\(\\alpha\\) is point-ultraweakly continuous and \\(h:G\\to M\\) is ultraweakly continuous and uniformly norm bounded, satisfying CO3. Its values need not be central or selfadjoint.\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "Here \\(G\\) is abelian, \\(\\alpha\\) is point-ultraweakly continuous and \\(h:G\\to M\\) is ultraweakly continuous and uniformly norm bounded, satisfying CO3. Its values need not be central or selfadjoint.\n"
        },
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          "full_statement_context": "<a id=\"equation-co3\"></a>\n\n\\[\nh_{st}=h_s+\\alpha_s(h_t).\n\\tag{CO3}\n\\]\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"equation-co3\"></a>\n\n\\[\nh_{st}=h_s+\\alpha_s(h_t).\n\\tag{CO3}\n\\]\n"
        }
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "<a id=\"co6\"></a>\n<a id=\"oa-flow.l125.co6\"></a>\n## CO6. Inspect an exact central correction in two blocks\n\nLet \\(M=M_2(\\mathbb C)\\oplus M_2(\\mathbb C)\\) and let the two-element group exchange the blocks. In units of \\(\\pi/32\\), take\n\n",
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          "full_conditions_and_proof": "<a id=\"co6\"></a>\n<a id=\"oa-flow.l125.co6\"></a>\n## CO6. Inspect an exact central correction in two blocks\n\nLet \\(M=M_2(\\mathbb C)\\oplus M_2(\\mathbb C)\\) and let the two-element group exchange the blocks. In units of \\(\\pi/32\\), take\n\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
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          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
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          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n",
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          "full_conditions_and_proof": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n",
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
        },
        {
          "source": "src/OA-FLOW-L125.md",
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
        },
        {
          "referenced_body_scope_id": "OA-FLOW.SMALLINNER.COCYCLE",
          "context_role": "standing_locally_compact_covariant_system_and_continuous_additive_cocycle_definition",
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          "source": "src/OA-FLOW-L125.md",
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          "full_statement_context": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n"
        },
        {
          "referenced_body_scope_id": "OA-FLOW.SMALLINNER.COBOUNDARY",
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          "full_statement_context": "<a id=\"smallinner-coboundary\"></a>\n<a id=\"oa-flow.smallinner.coboundary\"></a>\n### Bounded additive cocycles for abelian actions are coboundaries\n\nAssume throughout this section that $G$ is abelian, and suppose\n\n<a id=\"equation-p24\"></a>\n\n$$\nC:=\\sup_{s\\in G}\\lVert h(s)\\rVert<\\infty.\n\\tag{P24}\n$$\n\nFor $s\\in G$, define the ultraweakly continuous affine isometry\n\n<a id=\"equation-p25\"></a>\n\n$$\nT_s(x)=\\alpha_s(x)-h(s).\n\\tag{P25}\n$$\n\nThe cocycle identity gives\n\n<a id=\"equation-p26\"></a>\n\n$$\nT_sT_t(x)\n=\\alpha_{st}(x)-\\alpha_s(h(t))-h(s)\n=T_{st}(x).\n\\tag{P26}\n$$\n\nThus the $T_s$ commute.  The orbit of any $x\\in M$ is norm bounded, since\n\n<a id=\"equation-p27\"></a>\n\n$$\n\\lVert T_s(x)\\rVert\\le\\lVert x\\rVert+C.\n\\tag{P27}\n$$\n\nLet $K$ be its ultraweakly closed convex hull.  The closed ball of $M$, viewed\nas the dual of its predual, is ultraweakly compact; hence $K$ is a nonempty\ncompact convex set.  Moreover\n\n<a id=\"equation-p28\"></a>\n\n$$\nT_s\\{T_t(x):t\\in G\\}=\\{T_r(x):r\\in G\\},\n\\tag{P28}\n$$\n\nso every $T_s$ preserves $K$.  The Markov–Kakutani fixed-point theorem supplies\na common fixed point $k\\in K$:\n\n<a id=\"equation-p29\"></a>\n\n$$\nT_s(k)=k\n\\quad\\Longleftrightarrow\\quad\nh(s)=\\alpha_s(k)-k.\n\\tag{P29}\n$$\n\nTherefore every norm-bounded additive cocycle for the standing locally compact\nabelian action is a coboundary.  If the cocycle takes selfadjoint values in an\n$\\alpha$-invariant von Neumann subalgebra $A$, the argument may be run in $A$\nand $k$ replaced by $(k+k^*)/2$.  In particular, a central selfadjoint cocycle\nhas a central selfadjoint transfer element.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-coboundary\"></a>\n<a id=\"oa-flow.smallinner.coboundary\"></a>\n### Bounded additive cocycles for abelian actions are coboundaries\n\nAssume throughout this section that $G$ is abelian, and suppose\n\n<a id=\"equation-p24\"></a>\n\n$$\nC:=\\sup_{s\\in G}\\lVert h(s)\\rVert<\\infty.\n\\tag{P24}\n$$\n\nFor $s\\in G$, define the ultraweakly continuous affine isometry\n\n<a id=\"equation-p25\"></a>\n\n$$\nT_s(x)=\\alpha_s(x)-h(s).\n\\tag{P25}\n$$\n\nThe cocycle identity gives\n\n<a id=\"equation-p26\"></a>\n\n$$\nT_sT_t(x)\n=\\alpha_{st}(x)-\\alpha_s(h(t))-h(s)\n=T_{st}(x).\n\\tag{P26}\n$$\n\nThus the $T_s$ commute.  The orbit of any $x\\in M$ is norm bounded, since\n\n<a id=\"equation-p27\"></a>\n\n$$\n\\lVert T_s(x)\\rVert\\le\\lVert x\\rVert+C.\n\\tag{P27}\n$$\n\nLet $K$ be its ultraweakly closed convex hull.  The closed ball of $M$, viewed\nas the dual of its predual, is ultraweakly compact; hence $K$ is a nonempty\ncompact convex set.  Moreover\n\n<a id=\"equation-p28\"></a>\n\n$$\nT_s\\{T_t(x):t\\in G\\}=\\{T_r(x):r\\in G\\},\n\\tag{P28}\n$$\n\nso every $T_s$ preserves $K$.  The Markov–Kakutani fixed-point theorem supplies\na common fixed point $k\\in K$:\n\n<a id=\"equation-p29\"></a>\n\n$$\nT_s(k)=k\n\\quad\\Longleftrightarrow\\quad\nh(s)=\\alpha_s(k)-k.\n\\tag{P29}\n$$\n\nTherefore every norm-bounded additive cocycle for the standing locally compact\nabelian action is a coboundary.  If the cocycle takes selfadjoint values in an\n$\\alpha$-invariant von Neumann subalgebra $A$, the argument may be run in $A$\nand $k$ replaced by $(k+k^*)/2$.  In particular, a central selfadjoint cocycle\nhas a central selfadjoint transfer element.\n\n"
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          "full_statement_context": "<a id=\"smallinner-logarithm\"></a>\n<a id=\"oa-flow.smallinner.logarithm\"></a>\n### A strict logarithm branch turns the central unitary cocycle additive\n\nReturn to the locally compact abelian covariant system $(M,G,\\alpha)$.  Let\n$\\sigma\\in\\operatorname{Int}(M)$ commute with every $\\alpha_s$, and assume\n\n<a id=\"equation-p30\"></a>\n\n$$\n\\operatorname{Sp}(\\sigma)\\subset V(\\varepsilon),\n\\qquad 0<\\varepsilon<\\frac{\\pi}{4}.\n\\tag{P30}\n$$\n\nBy (P21), choose $v\\in\\mathcal U(M)$ such that\n\n<a id=\"equation-p31\"></a>\n\n$$\n\\sigma=\\operatorname{Ad}(v),\n\\qquad\n\\operatorname{Sp}_M(v)\\subset V(2\\varepsilon).\n\\tag{P31}\n$$\n\nSince $\\sigma$ commutes with $\\alpha_s$,\n\n<a id=\"equation-p32\"></a>\n\n$$\n\\operatorname{Ad}(v)\n=\\alpha_s\\operatorname{Ad}(v)\\alpha_s^{-1}\n=\\operatorname{Ad}(\\alpha_s(v)).\n\\tag{P32}\n$$\n\nTwo unitaries implement the same inner automorphism exactly when their quotient\nis central.  Hence\n\n<a id=\"equation-p33\"></a>\n\n$$\na_s=v^*\\alpha_s(v)\\in\\mathcal U(Z(M)),\n\\qquad\na_{st}=a_s\\alpha_s(a_t).\n\\tag{P33}\n$$\n\nLet $b=\\operatorname{Arg}(v)$ on the principal branch.  Compactness of\n$\\operatorname{Sp}_M(v)$ inside the open arc in (P31) gives\n\n<a id=\"equation-p34\"></a>\n\n$$\nb=b^*,\n\\qquad\nv=e^{ib},\n\\qquad\n\\lVert b\\rVert<2\\varepsilon.\n\\tag{P34}\n$$\n\nEquation (P33) says $\\alpha_s(v)=va_s$, so $v$ and $\\alpha_s(v)$ commute.\nTheir principal arguments $b$ and $\\alpha_s(b)$ therefore commute.  Put\n\n<a id=\"equation-p35\"></a>\n\n$$\nd_s=\\alpha_s(b)-b.\n\\tag{P35}\n$$\n\nThen\n\n<a id=\"equation-p36\"></a>\n\n$$\n\\lVert d_s\\rVert<4\\varepsilon<\\pi,\n\\qquad\na_s=e^{-ib}e^{i\\alpha_s(b)}=e^{id_s}.\n\\tag{P36}\n$$\n\nThe strict norm bound keeps the spectrum of $d_s$ inside the injectivity\ninterval of the exponential.  Consequently\n\n<a id=\"equation-p37\"></a>\n\n$$\nh(s):=\\operatorname{Arg}(a_s)=d_s=\\alpha_s(b)-b.\n\\tag{P37}\n$$\n\nBecause $a_s$ is central, functional calculus makes $h(s)$ central and\nselfadjoint.  Equation (P37), rather than a false global rule that logarithms\nturn arbitrary products into sums, gives directly\n\n<a id=\"equation-p38\"></a>\n\n$$\nh(st)\n=\\alpha_{st}(b)-b\n=h(s)+\\alpha_s(h(t)).\n\\tag{P38}\n$$\n\nThus $h:G\\to Z(M)_{\\mathrm{sa}}$ is an ultraweakly continuous additive\ncocycle, bounded by $4\\varepsilon$.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-logarithm\"></a>\n<a id=\"oa-flow.smallinner.logarithm\"></a>\n### A strict logarithm branch turns the central unitary cocycle additive\n\nReturn to the locally compact abelian covariant system $(M,G,\\alpha)$.  Let\n$\\sigma\\in\\operatorname{Int}(M)$ commute with every $\\alpha_s$, and assume\n\n<a id=\"equation-p30\"></a>\n\n$$\n\\operatorname{Sp}(\\sigma)\\subset V(\\varepsilon),\n\\qquad 0<\\varepsilon<\\frac{\\pi}{4}.\n\\tag{P30}\n$$\n\nBy (P21), choose $v\\in\\mathcal U(M)$ such that\n\n<a id=\"equation-p31\"></a>\n\n$$\n\\sigma=\\operatorname{Ad}(v),\n\\qquad\n\\operatorname{Sp}_M(v)\\subset V(2\\varepsilon).\n\\tag{P31}\n$$\n\nSince $\\sigma$ commutes with $\\alpha_s$,\n\n<a id=\"equation-p32\"></a>\n\n$$\n\\operatorname{Ad}(v)\n=\\alpha_s\\operatorname{Ad}(v)\\alpha_s^{-1}\n=\\operatorname{Ad}(\\alpha_s(v)).\n\\tag{P32}\n$$\n\nTwo unitaries implement the same inner automorphism exactly when their quotient\nis central.  Hence\n\n<a id=\"equation-p33\"></a>\n\n$$\na_s=v^*\\alpha_s(v)\\in\\mathcal U(Z(M)),\n\\qquad\na_{st}=a_s\\alpha_s(a_t).\n\\tag{P33}\n$$\n\nLet $b=\\operatorname{Arg}(v)$ on the principal branch.  Compactness of\n$\\operatorname{Sp}_M(v)$ inside the open arc in (P31) gives\n\n<a id=\"equation-p34\"></a>\n\n$$\nb=b^*,\n\\qquad\nv=e^{ib},\n\\qquad\n\\lVert b\\rVert<2\\varepsilon.\n\\tag{P34}\n$$\n\nEquation (P33) says $\\alpha_s(v)=va_s$, so $v$ and $\\alpha_s(v)$ commute.\nTheir principal arguments $b$ and $\\alpha_s(b)$ therefore commute.  Put\n\n<a id=\"equation-p35\"></a>\n\n$$\nd_s=\\alpha_s(b)-b.\n\\tag{P35}\n$$\n\nThen\n\n<a id=\"equation-p36\"></a>\n\n$$\n\\lVert d_s\\rVert<4\\varepsilon<\\pi,\n\\qquad\na_s=e^{-ib}e^{i\\alpha_s(b)}=e^{id_s}.\n\\tag{P36}\n$$\n\nThe strict norm bound keeps the spectrum of $d_s$ inside the injectivity\ninterval of the exponential.  Consequently\n\n<a id=\"equation-p37\"></a>\n\n$$\nh(s):=\\operatorname{Arg}(a_s)=d_s=\\alpha_s(b)-b.\n\\tag{P37}\n$$\n\nBecause $a_s$ is central, functional calculus makes $h(s)$ central and\nselfadjoint.  Equation (P37), rather than a false global rule that logarithms\nturn arbitrary products into sums, gives directly\n\n<a id=\"equation-p38\"></a>\n\n$$\nh(st)\n=\\alpha_{st}(b)-b\n=h(s)+\\alpha_s(h(t)).\n\\tag{P38}\n$$\n\nThus $h:G\\to Z(M)_{\\mathrm{sa}}$ is an ultraweakly continuous additive\ncocycle, bounded by $4\\varepsilon$.\n\n"
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          "full_statement_context": "Throughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "Throughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
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          "full_statement_context": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n",
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          "full_conditions_and_proof": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n"
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          "full_statement_context": "<a id=\"smallinner-coboundary\"></a>\n<a id=\"oa-flow.smallinner.coboundary\"></a>\n### Bounded additive cocycles for abelian actions are coboundaries\n\nAssume throughout this section that $G$ is abelian, and suppose\n\n<a id=\"equation-p24\"></a>\n\n$$\nC:=\\sup_{s\\in G}\\lVert h(s)\\rVert<\\infty.\n\\tag{P24}\n$$\n\nFor $s\\in G$, define the ultraweakly continuous affine isometry\n\n<a id=\"equation-p25\"></a>\n\n$$\nT_s(x)=\\alpha_s(x)-h(s).\n\\tag{P25}\n$$\n\nThe cocycle identity gives\n\n<a id=\"equation-p26\"></a>\n\n$$\nT_sT_t(x)\n=\\alpha_{st}(x)-\\alpha_s(h(t))-h(s)\n=T_{st}(x).\n\\tag{P26}\n$$\n\nThus the $T_s$ commute.  The orbit of any $x\\in M$ is norm bounded, since\n\n<a id=\"equation-p27\"></a>\n\n$$\n\\lVert T_s(x)\\rVert\\le\\lVert x\\rVert+C.\n\\tag{P27}\n$$\n\nLet $K$ be its ultraweakly closed convex hull.  The closed ball of $M$, viewed\nas the dual of its predual, is ultraweakly compact; hence $K$ is a nonempty\ncompact convex set.  Moreover\n\n<a id=\"equation-p28\"></a>\n\n$$\nT_s\\{T_t(x):t\\in G\\}=\\{T_r(x):r\\in G\\},\n\\tag{P28}\n$$\n\nso every $T_s$ preserves $K$.  The Markov–Kakutani fixed-point theorem supplies\na common fixed point $k\\in K$:\n\n<a id=\"equation-p29\"></a>\n\n$$\nT_s(k)=k\n\\quad\\Longleftrightarrow\\quad\nh(s)=\\alpha_s(k)-k.\n\\tag{P29}\n$$\n\nTherefore every norm-bounded additive cocycle for the standing locally compact\nabelian action is a coboundary.  If the cocycle takes selfadjoint values in an\n$\\alpha$-invariant von Neumann subalgebra $A$, the argument may be run in $A$\nand $k$ replaced by $(k+k^*)/2$.  In particular, a central selfadjoint cocycle\nhas a central selfadjoint transfer element.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-coboundary\"></a>\n<a id=\"oa-flow.smallinner.coboundary\"></a>\n### Bounded additive cocycles for abelian actions are coboundaries\n\nAssume throughout this section that $G$ is abelian, and suppose\n\n<a id=\"equation-p24\"></a>\n\n$$\nC:=\\sup_{s\\in G}\\lVert h(s)\\rVert<\\infty.\n\\tag{P24}\n$$\n\nFor $s\\in G$, define the ultraweakly continuous affine isometry\n\n<a id=\"equation-p25\"></a>\n\n$$\nT_s(x)=\\alpha_s(x)-h(s).\n\\tag{P25}\n$$\n\nThe cocycle identity gives\n\n<a id=\"equation-p26\"></a>\n\n$$\nT_sT_t(x)\n=\\alpha_{st}(x)-\\alpha_s(h(t))-h(s)\n=T_{st}(x).\n\\tag{P26}\n$$\n\nThus the $T_s$ commute.  The orbit of any $x\\in M$ is norm bounded, since\n\n<a id=\"equation-p27\"></a>\n\n$$\n\\lVert T_s(x)\\rVert\\le\\lVert x\\rVert+C.\n\\tag{P27}\n$$\n\nLet $K$ be its ultraweakly closed convex hull.  The closed ball of $M$, viewed\nas the dual of its predual, is ultraweakly compact; hence $K$ is a nonempty\ncompact convex set.  Moreover\n\n<a id=\"equation-p28\"></a>\n\n$$\nT_s\\{T_t(x):t\\in G\\}=\\{T_r(x):r\\in G\\},\n\\tag{P28}\n$$\n\nso every $T_s$ preserves $K$.  The Markov–Kakutani fixed-point theorem supplies\na common fixed point $k\\in K$:\n\n<a id=\"equation-p29\"></a>\n\n$$\nT_s(k)=k\n\\quad\\Longleftrightarrow\\quad\nh(s)=\\alpha_s(k)-k.\n\\tag{P29}\n$$\n\nTherefore every norm-bounded additive cocycle for the standing locally compact\nabelian action is a coboundary.  If the cocycle takes selfadjoint values in an\n$\\alpha$-invariant von Neumann subalgebra $A$, the argument may be run in $A$\nand $k$ replaced by $(k+k^*)/2$.  In particular, a central selfadjoint cocycle\nhas a central selfadjoint transfer element.\n\n"
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          "full_statement_context": "<a id=\"smallinner-logarithm\"></a>\n<a id=\"oa-flow.smallinner.logarithm\"></a>\n### A strict logarithm branch turns the central unitary cocycle additive\n\nReturn to the locally compact abelian covariant system $(M,G,\\alpha)$.  Let\n$\\sigma\\in\\operatorname{Int}(M)$ commute with every $\\alpha_s$, and assume\n\n<a id=\"equation-p30\"></a>\n\n$$\n\\operatorname{Sp}(\\sigma)\\subset V(\\varepsilon),\n\\qquad 0<\\varepsilon<\\frac{\\pi}{4}.\n\\tag{P30}\n$$\n\nBy (P21), choose $v\\in\\mathcal U(M)$ such that\n\n<a id=\"equation-p31\"></a>\n\n$$\n\\sigma=\\operatorname{Ad}(v),\n\\qquad\n\\operatorname{Sp}_M(v)\\subset V(2\\varepsilon).\n\\tag{P31}\n$$\n\nSince $\\sigma$ commutes with $\\alpha_s$,\n\n<a id=\"equation-p32\"></a>\n\n$$\n\\operatorname{Ad}(v)\n=\\alpha_s\\operatorname{Ad}(v)\\alpha_s^{-1}\n=\\operatorname{Ad}(\\alpha_s(v)).\n\\tag{P32}\n$$\n\nTwo unitaries implement the same inner automorphism exactly when their quotient\nis central.  Hence\n\n<a id=\"equation-p33\"></a>\n\n$$\na_s=v^*\\alpha_s(v)\\in\\mathcal U(Z(M)),\n\\qquad\na_{st}=a_s\\alpha_s(a_t).\n\\tag{P33}\n$$\n\nLet $b=\\operatorname{Arg}(v)$ on the principal branch.  Compactness of\n$\\operatorname{Sp}_M(v)$ inside the open arc in (P31) gives\n\n<a id=\"equation-p34\"></a>\n\n$$\nb=b^*,\n\\qquad\nv=e^{ib},\n\\qquad\n\\lVert b\\rVert<2\\varepsilon.\n\\tag{P34}\n$$\n\nEquation (P33) says $\\alpha_s(v)=va_s$, so $v$ and $\\alpha_s(v)$ commute.\nTheir principal arguments $b$ and $\\alpha_s(b)$ therefore commute.  Put\n\n<a id=\"equation-p35\"></a>\n\n$$\nd_s=\\alpha_s(b)-b.\n\\tag{P35}\n$$\n\nThen\n\n<a id=\"equation-p36\"></a>\n\n$$\n\\lVert d_s\\rVert<4\\varepsilon<\\pi,\n\\qquad\na_s=e^{-ib}e^{i\\alpha_s(b)}=e^{id_s}.\n\\tag{P36}\n$$\n\nThe strict norm bound keeps the spectrum of $d_s$ inside the injectivity\ninterval of the exponential.  Consequently\n\n<a id=\"equation-p37\"></a>\n\n$$\nh(s):=\\operatorname{Arg}(a_s)=d_s=\\alpha_s(b)-b.\n\\tag{P37}\n$$\n\nBecause $a_s$ is central, functional calculus makes $h(s)$ central and\nselfadjoint.  Equation (P37), rather than a false global rule that logarithms\nturn arbitrary products into sums, gives directly\n\n<a id=\"equation-p38\"></a>\n\n$$\nh(st)\n=\\alpha_{st}(b)-b\n=h(s)+\\alpha_s(h(t)).\n\\tag{P38}\n$$\n\nThus $h:G\\to Z(M)_{\\mathrm{sa}}$ is an ultraweakly continuous additive\ncocycle, bounded by $4\\varepsilon$.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-logarithm\"></a>\n<a id=\"oa-flow.smallinner.logarithm\"></a>\n### A strict logarithm branch turns the central unitary cocycle additive\n\nReturn to the locally compact abelian covariant system $(M,G,\\alpha)$.  Let\n$\\sigma\\in\\operatorname{Int}(M)$ commute with every $\\alpha_s$, and assume\n\n<a id=\"equation-p30\"></a>\n\n$$\n\\operatorname{Sp}(\\sigma)\\subset V(\\varepsilon),\n\\qquad 0<\\varepsilon<\\frac{\\pi}{4}.\n\\tag{P30}\n$$\n\nBy (P21), choose $v\\in\\mathcal U(M)$ such that\n\n<a id=\"equation-p31\"></a>\n\n$$\n\\sigma=\\operatorname{Ad}(v),\n\\qquad\n\\operatorname{Sp}_M(v)\\subset V(2\\varepsilon).\n\\tag{P31}\n$$\n\nSince $\\sigma$ commutes with $\\alpha_s$,\n\n<a id=\"equation-p32\"></a>\n\n$$\n\\operatorname{Ad}(v)\n=\\alpha_s\\operatorname{Ad}(v)\\alpha_s^{-1}\n=\\operatorname{Ad}(\\alpha_s(v)).\n\\tag{P32}\n$$\n\nTwo unitaries implement the same inner automorphism exactly when their quotient\nis central.  Hence\n\n<a id=\"equation-p33\"></a>\n\n$$\na_s=v^*\\alpha_s(v)\\in\\mathcal U(Z(M)),\n\\qquad\na_{st}=a_s\\alpha_s(a_t).\n\\tag{P33}\n$$\n\nLet $b=\\operatorname{Arg}(v)$ on the principal branch.  Compactness of\n$\\operatorname{Sp}_M(v)$ inside the open arc in (P31) gives\n\n<a id=\"equation-p34\"></a>\n\n$$\nb=b^*,\n\\qquad\nv=e^{ib},\n\\qquad\n\\lVert b\\rVert<2\\varepsilon.\n\\tag{P34}\n$$\n\nEquation (P33) says $\\alpha_s(v)=va_s$, so $v$ and $\\alpha_s(v)$ commute.\nTheir principal arguments $b$ and $\\alpha_s(b)$ therefore commute.  Put\n\n<a id=\"equation-p35\"></a>\n\n$$\nd_s=\\alpha_s(b)-b.\n\\tag{P35}\n$$\n\nThen\n\n<a id=\"equation-p36\"></a>\n\n$$\n\\lVert d_s\\rVert<4\\varepsilon<\\pi,\n\\qquad\na_s=e^{-ib}e^{i\\alpha_s(b)}=e^{id_s}.\n\\tag{P36}\n$$\n\nThe strict norm bound keeps the spectrum of $d_s$ inside the injectivity\ninterval of the exponential.  Consequently\n\n<a id=\"equation-p37\"></a>\n\n$$\nh(s):=\\operatorname{Arg}(a_s)=d_s=\\alpha_s(b)-b.\n\\tag{P37}\n$$\n\nBecause $a_s$ is central, functional calculus makes $h(s)$ central and\nselfadjoint.  Equation (P37), rather than a false global rule that logarithms\nturn arbitrary products into sums, gives directly\n\n<a id=\"equation-p38\"></a>\n\n$$\nh(st)\n=\\alpha_{st}(b)-b\n=h(s)+\\alpha_s(h(t)).\n\\tag{P38}\n$$\n\nThus $h:G\\to Z(M)_{\\mathrm{sa}}$ is an ultraweakly continuous additive\ncocycle, bounded by $4\\varepsilon$.\n\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
        },
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          "referenced_body_scope_id": "OA-FLOW.SMALLINNER.COCYCLE",
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          "source": "src/OA-FLOW-L125.md",
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          "full_statement_context": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n"
        },
        {
          "referenced_body_scope_id": "OA-FLOW.SMALLINNER.COBOUNDARY",
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          "full_statement_context": "<a id=\"smallinner-coboundary\"></a>\n<a id=\"oa-flow.smallinner.coboundary\"></a>\n### Bounded additive cocycles for abelian actions are coboundaries\n\nAssume throughout this section that $G$ is abelian, and suppose\n\n<a id=\"equation-p24\"></a>\n\n$$\nC:=\\sup_{s\\in G}\\lVert h(s)\\rVert<\\infty.\n\\tag{P24}\n$$\n\nFor $s\\in G$, define the ultraweakly continuous affine isometry\n\n<a id=\"equation-p25\"></a>\n\n$$\nT_s(x)=\\alpha_s(x)-h(s).\n\\tag{P25}\n$$\n\nThe cocycle identity gives\n\n<a id=\"equation-p26\"></a>\n\n$$\nT_sT_t(x)\n=\\alpha_{st}(x)-\\alpha_s(h(t))-h(s)\n=T_{st}(x).\n\\tag{P26}\n$$\n\nThus the $T_s$ commute.  The orbit of any $x\\in M$ is norm bounded, since\n\n<a id=\"equation-p27\"></a>\n\n$$\n\\lVert T_s(x)\\rVert\\le\\lVert x\\rVert+C.\n\\tag{P27}\n$$\n\nLet $K$ be its ultraweakly closed convex hull.  The closed ball of $M$, viewed\nas the dual of its predual, is ultraweakly compact; hence $K$ is a nonempty\ncompact convex set.  Moreover\n\n<a id=\"equation-p28\"></a>\n\n$$\nT_s\\{T_t(x):t\\in G\\}=\\{T_r(x):r\\in G\\},\n\\tag{P28}\n$$\n\nso every $T_s$ preserves $K$.  The Markov–Kakutani fixed-point theorem supplies\na common fixed point $k\\in K$:\n\n<a id=\"equation-p29\"></a>\n\n$$\nT_s(k)=k\n\\quad\\Longleftrightarrow\\quad\nh(s)=\\alpha_s(k)-k.\n\\tag{P29}\n$$\n\nTherefore every norm-bounded additive cocycle for the standing locally compact\nabelian action is a coboundary.  If the cocycle takes selfadjoint values in an\n$\\alpha$-invariant von Neumann subalgebra $A$, the argument may be run in $A$\nand $k$ replaced by $(k+k^*)/2$.  In particular, a central selfadjoint cocycle\nhas a central selfadjoint transfer element.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-coboundary\"></a>\n<a id=\"oa-flow.smallinner.coboundary\"></a>\n### Bounded additive cocycles for abelian actions are coboundaries\n\nAssume throughout this section that $G$ is abelian, and suppose\n\n<a id=\"equation-p24\"></a>\n\n$$\nC:=\\sup_{s\\in G}\\lVert h(s)\\rVert<\\infty.\n\\tag{P24}\n$$\n\nFor $s\\in G$, define the ultraweakly continuous affine isometry\n\n<a id=\"equation-p25\"></a>\n\n$$\nT_s(x)=\\alpha_s(x)-h(s).\n\\tag{P25}\n$$\n\nThe cocycle identity gives\n\n<a id=\"equation-p26\"></a>\n\n$$\nT_sT_t(x)\n=\\alpha_{st}(x)-\\alpha_s(h(t))-h(s)\n=T_{st}(x).\n\\tag{P26}\n$$\n\nThus the $T_s$ commute.  The orbit of any $x\\in M$ is norm bounded, since\n\n<a id=\"equation-p27\"></a>\n\n$$\n\\lVert T_s(x)\\rVert\\le\\lVert x\\rVert+C.\n\\tag{P27}\n$$\n\nLet $K$ be its ultraweakly closed convex hull.  The closed ball of $M$, viewed\nas the dual of its predual, is ultraweakly compact; hence $K$ is a nonempty\ncompact convex set.  Moreover\n\n<a id=\"equation-p28\"></a>\n\n$$\nT_s\\{T_t(x):t\\in G\\}=\\{T_r(x):r\\in G\\},\n\\tag{P28}\n$$\n\nso every $T_s$ preserves $K$.  The Markov–Kakutani fixed-point theorem supplies\na common fixed point $k\\in K$:\n\n<a id=\"equation-p29\"></a>\n\n$$\nT_s(k)=k\n\\quad\\Longleftrightarrow\\quad\nh(s)=\\alpha_s(k)-k.\n\\tag{P29}\n$$\n\nTherefore every norm-bounded additive cocycle for the standing locally compact\nabelian action is a coboundary.  If the cocycle takes selfadjoint values in an\n$\\alpha$-invariant von Neumann subalgebra $A$, the argument may be run in $A$\nand $k$ replaced by $(k+k^*)/2$.  In particular, a central selfadjoint cocycle\nhas a central selfadjoint transfer element.\n\n"
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          "full_statement_context": "<a id=\"smallinner-logarithm\"></a>\n<a id=\"oa-flow.smallinner.logarithm\"></a>\n### A strict logarithm branch turns the central unitary cocycle additive\n\nReturn to the locally compact abelian covariant system $(M,G,\\alpha)$.  Let\n$\\sigma\\in\\operatorname{Int}(M)$ commute with every $\\alpha_s$, and assume\n\n<a id=\"equation-p30\"></a>\n\n$$\n\\operatorname{Sp}(\\sigma)\\subset V(\\varepsilon),\n\\qquad 0<\\varepsilon<\\frac{\\pi}{4}.\n\\tag{P30}\n$$\n\nBy (P21), choose $v\\in\\mathcal U(M)$ such that\n\n<a id=\"equation-p31\"></a>\n\n$$\n\\sigma=\\operatorname{Ad}(v),\n\\qquad\n\\operatorname{Sp}_M(v)\\subset V(2\\varepsilon).\n\\tag{P31}\n$$\n\nSince $\\sigma$ commutes with $\\alpha_s$,\n\n<a id=\"equation-p32\"></a>\n\n$$\n\\operatorname{Ad}(v)\n=\\alpha_s\\operatorname{Ad}(v)\\alpha_s^{-1}\n=\\operatorname{Ad}(\\alpha_s(v)).\n\\tag{P32}\n$$\n\nTwo unitaries implement the same inner automorphism exactly when their quotient\nis central.  Hence\n\n<a id=\"equation-p33\"></a>\n\n$$\na_s=v^*\\alpha_s(v)\\in\\mathcal U(Z(M)),\n\\qquad\na_{st}=a_s\\alpha_s(a_t).\n\\tag{P33}\n$$\n\nLet $b=\\operatorname{Arg}(v)$ on the principal branch.  Compactness of\n$\\operatorname{Sp}_M(v)$ inside the open arc in (P31) gives\n\n<a id=\"equation-p34\"></a>\n\n$$\nb=b^*,\n\\qquad\nv=e^{ib},\n\\qquad\n\\lVert b\\rVert<2\\varepsilon.\n\\tag{P34}\n$$\n\nEquation (P33) says $\\alpha_s(v)=va_s$, so $v$ and $\\alpha_s(v)$ commute.\nTheir principal arguments $b$ and $\\alpha_s(b)$ therefore commute.  Put\n\n<a id=\"equation-p35\"></a>\n\n$$\nd_s=\\alpha_s(b)-b.\n\\tag{P35}\n$$\n\nThen\n\n<a id=\"equation-p36\"></a>\n\n$$\n\\lVert d_s\\rVert<4\\varepsilon<\\pi,\n\\qquad\na_s=e^{-ib}e^{i\\alpha_s(b)}=e^{id_s}.\n\\tag{P36}\n$$\n\nThe strict norm bound keeps the spectrum of $d_s$ inside the injectivity\ninterval of the exponential.  Consequently\n\n<a id=\"equation-p37\"></a>\n\n$$\nh(s):=\\operatorname{Arg}(a_s)=d_s=\\alpha_s(b)-b.\n\\tag{P37}\n$$\n\nBecause $a_s$ is central, functional calculus makes $h(s)$ central and\nselfadjoint.  Equation (P37), rather than a false global rule that logarithms\nturn arbitrary products into sums, gives directly\n\n<a id=\"equation-p38\"></a>\n\n$$\nh(st)\n=\\alpha_{st}(b)-b\n=h(s)+\\alpha_s(h(t)).\n\\tag{P38}\n$$\n\nThus $h:G\\to Z(M)_{\\mathrm{sa}}$ is an ultraweakly continuous additive\ncocycle, bounded by $4\\varepsilon$.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-logarithm\"></a>\n<a id=\"oa-flow.smallinner.logarithm\"></a>\n### A strict logarithm branch turns the central unitary cocycle additive\n\nReturn to the locally compact abelian covariant system $(M,G,\\alpha)$.  Let\n$\\sigma\\in\\operatorname{Int}(M)$ commute with every $\\alpha_s$, and assume\n\n<a id=\"equation-p30\"></a>\n\n$$\n\\operatorname{Sp}(\\sigma)\\subset V(\\varepsilon),\n\\qquad 0<\\varepsilon<\\frac{\\pi}{4}.\n\\tag{P30}\n$$\n\nBy (P21), choose $v\\in\\mathcal U(M)$ such that\n\n<a id=\"equation-p31\"></a>\n\n$$\n\\sigma=\\operatorname{Ad}(v),\n\\qquad\n\\operatorname{Sp}_M(v)\\subset V(2\\varepsilon).\n\\tag{P31}\n$$\n\nSince $\\sigma$ commutes with $\\alpha_s$,\n\n<a id=\"equation-p32\"></a>\n\n$$\n\\operatorname{Ad}(v)\n=\\alpha_s\\operatorname{Ad}(v)\\alpha_s^{-1}\n=\\operatorname{Ad}(\\alpha_s(v)).\n\\tag{P32}\n$$\n\nTwo unitaries implement the same inner automorphism exactly when their quotient\nis central.  Hence\n\n<a id=\"equation-p33\"></a>\n\n$$\na_s=v^*\\alpha_s(v)\\in\\mathcal U(Z(M)),\n\\qquad\na_{st}=a_s\\alpha_s(a_t).\n\\tag{P33}\n$$\n\nLet $b=\\operatorname{Arg}(v)$ on the principal branch.  Compactness of\n$\\operatorname{Sp}_M(v)$ inside the open arc in (P31) gives\n\n<a id=\"equation-p34\"></a>\n\n$$\nb=b^*,\n\\qquad\nv=e^{ib},\n\\qquad\n\\lVert b\\rVert<2\\varepsilon.\n\\tag{P34}\n$$\n\nEquation (P33) says $\\alpha_s(v)=va_s$, so $v$ and $\\alpha_s(v)$ commute.\nTheir principal arguments $b$ and $\\alpha_s(b)$ therefore commute.  Put\n\n<a id=\"equation-p35\"></a>\n\n$$\nd_s=\\alpha_s(b)-b.\n\\tag{P35}\n$$\n\nThen\n\n<a id=\"equation-p36\"></a>\n\n$$\n\\lVert d_s\\rVert<4\\varepsilon<\\pi,\n\\qquad\na_s=e^{-ib}e^{i\\alpha_s(b)}=e^{id_s}.\n\\tag{P36}\n$$\n\nThe strict norm bound keeps the spectrum of $d_s$ inside the injectivity\ninterval of the exponential.  Consequently\n\n<a id=\"equation-p37\"></a>\n\n$$\nh(s):=\\operatorname{Arg}(a_s)=d_s=\\alpha_s(b)-b.\n\\tag{P37}\n$$\n\nBecause $a_s$ is central, functional calculus makes $h(s)$ central and\nselfadjoint.  Equation (P37), rather than a false global rule that logarithms\nturn arbitrary products into sums, gives directly\n\n<a id=\"equation-p38\"></a>\n\n$$\nh(st)\n=\\alpha_{st}(b)-b\n=h(s)+\\alpha_s(h(t)).\n\\tag{P38}\n$$\n\nThus $h:G\\to Z(M)_{\\mathrm{sa}}$ is an ultraweakly continuous additive\ncocycle, bounded by $4\\varepsilon$.\n\n"
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          "full_statement_context": "Throughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "Throughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n"
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          "full_statement_context": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"l125-historical-setting\"></a>\n<a id=\"oa-flow.l125.historical.setting\"></a>\n## Phase localization and abelian fixed-point route\n\nCO3 supplies the uniform compact-set subdivision used below, CO5 supplies the complete commuting affine fixed-point proof, and CO2 proves the precise logarithm branch. In P12–P13 take \\(\\delta+\\varepsilon<\\pi\\), as in CO4; a radius at least \\(\\pi\\) gives the whole circle and needs no \\(V(r)\\) notation outside its defined range. Its group hypotheses remain those actually stated, even though the central order route works for a larger group class.\n\n## Phase localization and fixed small-spectrum implementers\n\nA small operator spectrum for an inner automorphism can be converted into a\nsmall spectrum for one of its implementing unitaries.  If the automorphism also\ncommutes with an abelian action, a central logarithmic correction makes that\nimplementer fixed by the action.  The proof has two delicate points: the\ncentral spectral pieces must form an actually orthogonal partition, and the\nprincipal logarithm may be made additive only after a strict branch estimate.\n\nLet $M$ be a nonzero von Neumann algebra.  For $0<r<\\pi$, write\n\n<a id=\"equation-p1\"></a>\n\n$$\nV(r)=\\{e^{it}:|t|<r\\}\\subset\\mathbb T,\n\\tag{P1}\n$$\n\nand let $d_{\\mathbb T}$ denote circular angular distance.  For a unitary\n$u\\in M$, put\n\n<a id=\"equation-p2\"></a>\n\n$$\np(\\theta,r)\n=1_{\\{z\\in\\mathbb T:d_{\\mathbb T}(z,e^{i\\theta})\\le r\\}}(u).\n\\tag{P2}\n$$\n\nThe symbol $\\operatorname{Sp}(\\operatorname{Ad}(u))$ below denotes the\nordinary Banach-operator spectrum of $\\operatorname{Ad}(u)$ on $M$; it is not\nthe dual-group spectrum of an action.\n\n"
        },
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          "full_statement_context": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-cocycle\"></a>\n<a id=\"oa-flow.smallinner.cocycle\"></a>\n### Additive cocycles and coboundaries\n\nLet $G$ be a locally compact group and let\n$\\alpha:G\\to\\operatorname{Aut}(M)$ be point-ultraweakly continuous.  In\nmultiplicative notation, an **additive one-cocycle** is an ultraweakly\ncontinuous map $h:G\\to M$ satisfying\n\n<a id=\"equation-p22\"></a>\n\n$$\nh(st)=h(s)+\\alpha_s(h(t))\n\\qquad(s,t\\in G).\n\\tag{P22}\n$$\n\nIt is a **coboundary** if one element $k\\in M$ satisfies\n\n<a id=\"equation-p23\"></a>\n\n$$\nh(s)=\\alpha_s(k)-k\n\\qquad(s\\in G).\n\\tag{P23}\n$$\n\nThese definitions make sense for nonabelian $G$.  The bounded-cocycle result\nproved next uses the standing abelian hypothesis, because its affine maps must\ncommute.\n\n"
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          "full_statement_context": "<a id=\"smallinner-coboundary\"></a>\n<a id=\"oa-flow.smallinner.coboundary\"></a>\n### Bounded additive cocycles for abelian actions are coboundaries\n\nAssume throughout this section that $G$ is abelian, and suppose\n\n<a id=\"equation-p24\"></a>\n\n$$\nC:=\\sup_{s\\in G}\\lVert h(s)\\rVert<\\infty.\n\\tag{P24}\n$$\n\nFor $s\\in G$, define the ultraweakly continuous affine isometry\n\n<a id=\"equation-p25\"></a>\n\n$$\nT_s(x)=\\alpha_s(x)-h(s).\n\\tag{P25}\n$$\n\nThe cocycle identity gives\n\n<a id=\"equation-p26\"></a>\n\n$$\nT_sT_t(x)\n=\\alpha_{st}(x)-\\alpha_s(h(t))-h(s)\n=T_{st}(x).\n\\tag{P26}\n$$\n\nThus the $T_s$ commute.  The orbit of any $x\\in M$ is norm bounded, since\n\n<a id=\"equation-p27\"></a>\n\n$$\n\\lVert T_s(x)\\rVert\\le\\lVert x\\rVert+C.\n\\tag{P27}\n$$\n\nLet $K$ be its ultraweakly closed convex hull.  The closed ball of $M$, viewed\nas the dual of its predual, is ultraweakly compact; hence $K$ is a nonempty\ncompact convex set.  Moreover\n\n<a id=\"equation-p28\"></a>\n\n$$\nT_s\\{T_t(x):t\\in G\\}=\\{T_r(x):r\\in G\\},\n\\tag{P28}\n$$\n\nso every $T_s$ preserves $K$.  The Markov–Kakutani fixed-point theorem supplies\na common fixed point $k\\in K$:\n\n<a id=\"equation-p29\"></a>\n\n$$\nT_s(k)=k\n\\quad\\Longleftrightarrow\\quad\nh(s)=\\alpha_s(k)-k.\n\\tag{P29}\n$$\n\nTherefore every norm-bounded additive cocycle for the standing locally compact\nabelian action is a coboundary.  If the cocycle takes selfadjoint values in an\n$\\alpha$-invariant von Neumann subalgebra $A$, the argument may be run in $A$\nand $k$ replaced by $(k+k^*)/2$.  In particular, a central selfadjoint cocycle\nhas a central selfadjoint transfer element.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "<a id=\"smallinner-coboundary\"></a>\n<a id=\"oa-flow.smallinner.coboundary\"></a>\n### Bounded additive cocycles for abelian actions are coboundaries\n\nAssume throughout this section that $G$ is abelian, and suppose\n\n<a id=\"equation-p24\"></a>\n\n$$\nC:=\\sup_{s\\in G}\\lVert h(s)\\rVert<\\infty.\n\\tag{P24}\n$$\n\nFor $s\\in G$, define the ultraweakly continuous affine isometry\n\n<a id=\"equation-p25\"></a>\n\n$$\nT_s(x)=\\alpha_s(x)-h(s).\n\\tag{P25}\n$$\n\nThe cocycle identity gives\n\n<a id=\"equation-p26\"></a>\n\n$$\nT_sT_t(x)\n=\\alpha_{st}(x)-\\alpha_s(h(t))-h(s)\n=T_{st}(x).\n\\tag{P26}\n$$\n\nThus the $T_s$ commute.  The orbit of any $x\\in M$ is norm bounded, since\n\n<a id=\"equation-p27\"></a>\n\n$$\n\\lVert T_s(x)\\rVert\\le\\lVert x\\rVert+C.\n\\tag{P27}\n$$\n\nLet $K$ be its ultraweakly closed convex hull.  The closed ball of $M$, viewed\nas the dual of its predual, is ultraweakly compact; hence $K$ is a nonempty\ncompact convex set.  Moreover\n\n<a id=\"equation-p28\"></a>\n\n$$\nT_s\\{T_t(x):t\\in G\\}=\\{T_r(x):r\\in G\\},\n\\tag{P28}\n$$\n\nso every $T_s$ preserves $K$.  The Markov–Kakutani fixed-point theorem supplies\na common fixed point $k\\in K$:\n\n<a id=\"equation-p29\"></a>\n\n$$\nT_s(k)=k\n\\quad\\Longleftrightarrow\\quad\nh(s)=\\alpha_s(k)-k.\n\\tag{P29}\n$$\n\nTherefore every norm-bounded additive cocycle for the standing locally compact\nabelian action is a coboundary.  If the cocycle takes selfadjoint values in an\n$\\alpha$-invariant von Neumann subalgebra $A$, the argument may be run in $A$\nand $k$ replaced by $(k+k^*)/2$.  In particular, a central selfadjoint cocycle\nhas a central selfadjoint transfer element.\n\n"
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          "full_statement_context": "<a id=\"smallinner-logarithm\"></a>\n<a id=\"oa-flow.smallinner.logarithm\"></a>\n### A strict logarithm branch turns the central unitary cocycle additive\n\nReturn to the locally compact abelian covariant system $(M,G,\\alpha)$.  Let\n$\\sigma\\in\\operatorname{Int}(M)$ commute with every $\\alpha_s$, and assume\n\n<a id=\"equation-p30\"></a>\n\n$$\n\\operatorname{Sp}(\\sigma)\\subset V(\\varepsilon),\n\\qquad 0<\\varepsilon<\\frac{\\pi}{4}.\n\\tag{P30}\n$$\n\nBy (P21), choose $v\\in\\mathcal U(M)$ such that\n\n<a id=\"equation-p31\"></a>\n\n$$\n\\sigma=\\operatorname{Ad}(v),\n\\qquad\n\\operatorname{Sp}_M(v)\\subset V(2\\varepsilon).\n\\tag{P31}\n$$\n\nSince $\\sigma$ commutes with $\\alpha_s$,\n\n<a id=\"equation-p32\"></a>\n\n$$\n\\operatorname{Ad}(v)\n=\\alpha_s\\operatorname{Ad}(v)\\alpha_s^{-1}\n=\\operatorname{Ad}(\\alpha_s(v)).\n\\tag{P32}\n$$\n\nTwo unitaries implement the same inner automorphism exactly when their quotient\nis central.  Hence\n\n<a id=\"equation-p33\"></a>\n\n$$\na_s=v^*\\alpha_s(v)\\in\\mathcal U(Z(M)),\n\\qquad\na_{st}=a_s\\alpha_s(a_t).\n\\tag{P33}\n$$\n\nLet $b=\\operatorname{Arg}(v)$ on the principal branch.  Compactness of\n$\\operatorname{Sp}_M(v)$ inside the open arc in (P31) gives\n\n<a id=\"equation-p34\"></a>\n\n$$\nb=b^*,\n\\qquad\nv=e^{ib},\n\\qquad\n\\lVert b\\rVert<2\\varepsilon.\n\\tag{P34}\n$$\n\nEquation (P33) says $\\alpha_s(v)=va_s$, so $v$ and $\\alpha_s(v)$ commute.\nTheir principal arguments $b$ and $\\alpha_s(b)$ therefore commute.  Put\n\n<a id=\"equation-p35\"></a>\n\n$$\nd_s=\\alpha_s(b)-b.\n\\tag{P35}\n$$\n\nThen\n\n<a id=\"equation-p36\"></a>\n\n$$\n\\lVert d_s\\rVert<4\\varepsilon<\\pi,\n\\qquad\na_s=e^{-ib}e^{i\\alpha_s(b)}=e^{id_s}.\n\\tag{P36}\n$$\n\nThe strict norm bound keeps the spectrum of $d_s$ inside the injectivity\ninterval of the exponential.  Consequently\n\n<a id=\"equation-p37\"></a>\n\n$$\nh(s):=\\operatorname{Arg}(a_s)=d_s=\\alpha_s(b)-b.\n\\tag{P37}\n$$\n\nBecause $a_s$ is central, functional calculus makes $h(s)$ central and\nselfadjoint.  Equation (P37), rather than a false global rule that logarithms\nturn arbitrary products into sums, gives directly\n\n<a id=\"equation-p38\"></a>\n\n$$\nh(st)\n=\\alpha_{st}(b)-b\n=h(s)+\\alpha_s(h(t)).\n\\tag{P38}\n$$\n\nThus $h:G\\to Z(M)_{\\mathrm{sa}}$ is an ultraweakly continuous additive\ncocycle, bounded by $4\\varepsilon$.\n\n",
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          "full_conditions_and_proof": "<a id=\"smallinner-logarithm\"></a>\n<a id=\"oa-flow.smallinner.logarithm\"></a>\n### A strict logarithm branch turns the central unitary cocycle additive\n\nReturn to the locally compact abelian covariant system $(M,G,\\alpha)$.  Let\n$\\sigma\\in\\operatorname{Int}(M)$ commute with every $\\alpha_s$, and assume\n\n<a id=\"equation-p30\"></a>\n\n$$\n\\operatorname{Sp}(\\sigma)\\subset V(\\varepsilon),\n\\qquad 0<\\varepsilon<\\frac{\\pi}{4}.\n\\tag{P30}\n$$\n\nBy (P21), choose $v\\in\\mathcal U(M)$ such that\n\n<a id=\"equation-p31\"></a>\n\n$$\n\\sigma=\\operatorname{Ad}(v),\n\\qquad\n\\operatorname{Sp}_M(v)\\subset V(2\\varepsilon).\n\\tag{P31}\n$$\n\nSince $\\sigma$ commutes with $\\alpha_s$,\n\n<a id=\"equation-p32\"></a>\n\n$$\n\\operatorname{Ad}(v)\n=\\alpha_s\\operatorname{Ad}(v)\\alpha_s^{-1}\n=\\operatorname{Ad}(\\alpha_s(v)).\n\\tag{P32}\n$$\n\nTwo unitaries implement the same inner automorphism exactly when their quotient\nis central.  Hence\n\n<a id=\"equation-p33\"></a>\n\n$$\na_s=v^*\\alpha_s(v)\\in\\mathcal U(Z(M)),\n\\qquad\na_{st}=a_s\\alpha_s(a_t).\n\\tag{P33}\n$$\n\nLet $b=\\operatorname{Arg}(v)$ on the principal branch.  Compactness of\n$\\operatorname{Sp}_M(v)$ inside the open arc in (P31) gives\n\n<a id=\"equation-p34\"></a>\n\n$$\nb=b^*,\n\\qquad\nv=e^{ib},\n\\qquad\n\\lVert b\\rVert<2\\varepsilon.\n\\tag{P34}\n$$\n\nEquation (P33) says $\\alpha_s(v)=va_s$, so $v$ and $\\alpha_s(v)$ commute.\nTheir principal arguments $b$ and $\\alpha_s(b)$ therefore commute.  Put\n\n<a id=\"equation-p35\"></a>\n\n$$\nd_s=\\alpha_s(b)-b.\n\\tag{P35}\n$$\n\nThen\n\n<a id=\"equation-p36\"></a>\n\n$$\n\\lVert d_s\\rVert<4\\varepsilon<\\pi,\n\\qquad\na_s=e^{-ib}e^{i\\alpha_s(b)}=e^{id_s}.\n\\tag{P36}\n$$\n\nThe strict norm bound keeps the spectrum of $d_s$ inside the injectivity\ninterval of the exponential.  Consequently\n\n<a id=\"equation-p37\"></a>\n\n$$\nh(s):=\\operatorname{Arg}(a_s)=d_s=\\alpha_s(b)-b.\n\\tag{P37}\n$$\n\nBecause $a_s$ is central, functional calculus makes $h(s)$ central and\nselfadjoint.  Equation (P37), rather than a false global rule that logarithms\nturn arbitrary products into sums, gives directly\n\n<a id=\"equation-p38\"></a>\n\n$$\nh(st)\n=\\alpha_{st}(b)-b\n=h(s)+\\alpha_s(h(t)).\n\\tag{P38}\n$$\n\nThus $h:G\\to Z(M)_{\\mathrm{sa}}$ is an ultraweakly continuous additive\ncocycle, bounded by $4\\varepsilon$.\n\n"
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          "full_statement_context": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n",
          "usage": "Exact declared context; definition references add no proved-premise edge.",
          "full_conditions_and_proof": "# A central order correction fixes the implementer and retains its bound\n\nAn inner automorphism with small Banach-operator spectrum has an implementer with a small principal logarithm. A commuting group can then be removed from that implementer by a central correction. We first prove the order construction that makes this correction possible for an arbitrary group. We next construct the small logarithm by spectral separation. The independent compact convex argument for a general abelian bounded cocycle and the entire earlier P argument remain available as alternative routes.\n\n*Original exposition and illustrations: CC0-1.0 to the extent of rights held; existing component and font terms apply.*\n\n<a id=\"l125-inputs\"></a>\n<a id=\"oa-flow.l125.setting\"></a>\n## Full hypotheses and earlier proofs\n\nThroughout, \\(M\\ne0\\) is a concrete von Neumann algebra on an arbitrary complex Hilbert space. The center is \\(Z(M)\\). A group action \\(\\alpha:G\\to\\operatorname{Aut}(M)\\) uses multiplicative notation. The central order results impose no topology, commutativity or amenability on \\(G\\). The separate general noncentral cocycle theorem requires \\(G\\) abelian. When continuity is mentioned it means point-ultraweak continuity, and cocycle continuity uses the ultraweak topology.\n\nFor a unitary \\(v\\), the notation \\(S=\\operatorname{Ad}(v)\\) denotes a bounded linear isometry of the Banach space \\(M\\), with isometric inverse. Its \\(\\operatorname{Sp}(S)\\) is the ordinary Banach-operator spectrum; \\(\\operatorname{Sp}_M(v)\\) is the spectrum of the unitary in its algebra. These are not action spectra. We use \\(V(r)=\\{e^{it}:|t|<r\\}\\), with angular distance on the circle, and the principal argument with values in \\((-\\pi,\\pi)\\) wherever its branch is defined.\n\nThe exact complete earlier inputs are [CF1 compactness, choice and norm series](OA-FLOW-CF.md#oa-flow.cf.1), [CF2 Banach inverses and resolvent continuity](OA-FLOW-CF.md#oa-flow.cf.2), [CF4 product compactness](OA-FLOW-CF.md#oa-flow.cf.4), [CF6 continuous calculus](OA-FLOW-CF.md#oa-flow.cf.6), [CF7 positive order](OA-FLOW-CF.md#oa-flow.cf.7), [CF8 arbitrary Hilbert operators](OA-FLOW-CF.md#oa-flow.cf.8), [SF0 commutant-unitary test](OA-FLOW-SF.md#oa-flow.sf.sf0), [SB3 complete unitary Borel calculus](OA-FLOW-SF.md#oa-flow.sf.sb3), [CP6 concrete predual](OA-FLOW-CP.md#oa-flow.cp.6), [NF6 normal positive maps](OA-FLOW-NF.md#oa-flow.nf.6), [PC1 corners and arbitrary joins](OA-FLOW-PC.md#oa-flow.projection.pc1), and [PC2 central supports](OA-FLOW-PC.md#oa-flow.projection.pc2).\n\nSB3 constructs the unitary calculus for an arbitrary cyclic family. PC1–2 apply without restrictions on dimension or cardinality.\n\n"
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          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
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      "id": "OA-FLOW.L126.CORNER.CENTER",
      "unit": "OA-FLOW-L126",
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      "prerequisites": [
        "OA-FLOW.PC.2",
        "OA-FLOW.PC.4",
        "OA-FLOW.GCC.SETTING"
      ],
      "may_be_used_as_earlier_proved_premise": true,
      "proof_available_after_line": 36,
      "source_level_hypothesis_ranges": [
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 17,
          "end_line": 17,
          "full_statement_context": "Let $0\\ne e\\in\\operatorname{Proj}(F)$. Its ambient central support is the least central projection dominating it. Each $\\alpha_s$ permutes such projections, so\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        }
      ]
    },
    {
      "id": "OA-FLOW.L126.LOCAL.RECOGNITION",
      "unit": "OA-FLOW-L126",
      "source_file": "src/OA-FLOW-L126.md",
      "source_sha256": "01c4e943b0b161d3febc126f4d6dc380ef2646ead7888cb07c111728ce15635f",
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      "prerequisites": [
        "OA-FLOW.L126.CORNER.CENTER",
        "OA-FLOW.OPSP.FORMULA",
        "OA-FLOW.CONNES.SUBGROUP",
        "OA-FLOW.FULLCORNER.INNER",
        "OA-FLOW.L124.CE5",
        "OA-FLOW.L125.CO4"
      ],
      "may_be_used_as_earlier_proved_premise": true,
      "proof_available_after_line": 78,
      "source_level_hypothesis_ranges": [
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 37,
          "end_line": 46,
          "full_statement_context": "<a id=\"lc1\"></a>\n<a id=\"oa-flow.l126.lc1\"></a>\n## LC1. A small cyclic spectrum supplies a central fixed lift\n\nFix $t\\in G$ and put $\\sigma=\\alpha_t$. Suppose there exist a nonzero fixed projection $e$ and a radius $0<r<\\pi/4$ with\n<a id=\"equation-lc4\"></a>\n\\[\n\\operatorname{Sp}_{\\mathcal L(eMe)}(\\sigma^e)\\subset V(r).\n\\tag{LC4}\n\\]\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        }
      ]
    },
    {
      "id": "OA-FLOW.L126.COMPACT.SELECTION",
      "unit": "OA-FLOW-L126",
      "source_file": "src/OA-FLOW-L126.md",
      "source_sha256": "01c4e943b0b161d3febc126f4d6dc380ef2646ead7888cb07c111728ce15635f",
      "reader": "OA-FLOW-L126.html#lc2",
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      "end_line": 134,
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      "prerequisites": [
        "OA-FLOW.CONNES.ABSORPTION",
        "OA-FLOW.CONNES.SUBGROUP",
        "OA-FLOW.GCC.SETTING",
        "OA-FLOW.GCC.INTERSECTION",
        "OA-FLOW.L121.SC0",
        "OA-FLOW.DIRECTED.THICKENING",
        "OA-FLOW.HR.TOPOLOGY"
      ],
      "may_be_used_as_earlier_proved_premise": true,
      "proof_available_after_line": 134,
      "source_level_hypothesis_ranges": [
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 79,
          "end_line": 89,
          "full_statement_context": "<a id=\"lc2\"></a>\n<a id=\"oa-flow.l126.lc2\"></a>\n## LC2. Compact saturated thickenings select a corner\n\nNow assume precisely\n<a id=\"equation-lc9\"></a>\n\\[\nS=\\pi(\\operatorname{Sp}(\\alpha))\\text{ is compact},\n\\qquad \\pi:H\\longrightarrow H/\\Gamma.\n\\tag{LC9}\n\\]\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        }
      ]
    },
    {
      "id": "OA-FLOW.L126.CENTRAL.FIXED.TIMES",
      "unit": "OA-FLOW-L126",
      "source_file": "src/OA-FLOW-L126.md",
      "source_sha256": "01c4e943b0b161d3febc126f4d6dc380ef2646ead7888cb07c111728ce15635f",
      "reader": "OA-FLOW-L126.html#lc3",
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      "end_line": 164,
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      "prerequisites": [
        "OA-FLOW.L126.LOCAL.RECOGNITION",
        "OA-FLOW.L126.COMPACT.SELECTION",
        "OA-FLOW.OPSP.FORMULA",
        "OA-FLOW.AT.3",
        "OA-FLOW.GCC.SETTING",
        "OA-FLOW.L115.CONVENTIONS",
        "OA-FLOW.L122.DIRECTANNIHILATOR"
      ],
      "may_be_used_as_earlier_proved_premise": true,
      "proof_available_after_line": 164,
      "source_level_hypothesis_ranges": [
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 79,
          "end_line": 89,
          "full_statement_context": "<a id=\"lc2\"></a>\n<a id=\"oa-flow.l126.lc2\"></a>\n## LC2. Compact saturated thickenings select a corner\n\nNow assume precisely\n<a id=\"equation-lc9\"></a>\n\\[\nS=\\pi(\\operatorname{Sp}(\\alpha))\\text{ is compact},\n\\qquad \\pi:H\\longrightarrow H/\\Gamma.\n\\tag{LC9}\n\\]\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 135,
          "end_line": 145,
          "full_statement_context": "<a id=\"lc3\"></a>\n<a id=\"oa-flow.l126.lc3\"></a>\n## LC3. The annihilator is exactly the centrally implemented times\n\nTake $t\\in\\Gamma^\\perp$. The continuous character $p\\mapsto(t,p)$ is constant on $\\Gamma$-cosets, so the quotient topology supplies a continuous character $\\chi_t:H/\\Gamma\\to\\mathbb T$. Choose radii\n<a id=\"equation-lc15\"></a>\n\\[\n0<a<b<\\pi/4,\n\\qquad O=\\chi_t^{-1}(V(a)).\n\\tag{LC15}\n\\]\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        }
      ]
    },
    {
      "id": "OA-FLOW.L126.EXACT.MODEL",
      "unit": "OA-FLOW-L126",
      "source_file": "src/OA-FLOW-L126.md",
      "source_sha256": "01c4e943b0b161d3febc126f4d6dc380ef2646ead7888cb07c111728ce15635f",
      "reader": "OA-FLOW-L126.html#lc4",
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      "end_line": 189,
      "range_sha256": "b3e8b3f4d9101ca9f75df0971e908e16850463f422cdb9b0a448667da2d2c3a9",
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      "prerequisites": [
        "OA-FLOW.L126.CENTRAL.FIXED.TIMES"
      ],
      "may_be_used_as_earlier_proved_premise": false,
      "proof_available_after_line": 189,
      "source_level_hypothesis_ranges": [
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 165,
          "end_line": 175,
          "full_statement_context": "<a id=\"lc4\"></a>\n<a id=\"oa-flow.l126.lc4\"></a>\n## LC4. An exact finite example and the meaning of the chosen phase\n\nLet $M=M_3(\\mathbb C)$, $G=\\mathbb R$, and\n<a id=\"equation-lc18\"></a>\n\\[\nW_s=\\operatorname{diag}(1,e^{is},e^{2is}),\\qquad\n\\alpha_s=\\operatorname{Ad}(W_s),\\qquad e=E_{22}.\n\\tag{LC18}\n\\]\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        }
      ]
    },
    {
      "id": "OA-FLOW.L126.SOURCE.COMPARISON",
      "unit": "OA-FLOW-L126",
      "source_file": "src/OA-FLOW-L126.md",
      "source_sha256": "01c4e943b0b161d3febc126f4d6dc380ef2646ead7888cb07c111728ce15635f",
      "reader": "OA-FLOW-L126.html#l126-source-comparison",
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      "prerequisites": [],
      "may_be_used_as_earlier_proved_premise": false,
      "proof_available_after_line": 198,
      "source_level_hypothesis_ranges": []
    },
    {
      "id": "OA-FLOW.L126.HIST.SETTING",
      "unit": "OA-FLOW-L126",
      "source_file": "src/OA-FLOW-L126.md",
      "source_sha256": "01c4e943b0b161d3febc126f4d6dc380ef2646ead7888cb07c111728ce15635f",
      "reader": "OA-FLOW-L126.html#historical-alternative",
      "start_line": 212,
      "end_line": 251,
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      "prerequisites": [],
      "may_be_used_as_earlier_proved_premise": false,
      "proof_available_after_line": 251,
      "source_level_hypothesis_ranges": [
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 224,
          "end_line": 251,
          "full_statement_context": "Throughout, $G$ is a locally compact Hausdorff abelian group,\n$H=\\widehat G$, $M$ is a nonzero von Neumann algebra, and\n$\\alpha:G\\to\\operatorname{Aut}(M)$ is point-ultraweakly continuous and\ncentrally ergodic.  Put\n\n<a id=\"equation-q1\"></a>\n$$\n\\Gamma=\\Gamma(\\alpha),\n\\qquad\nD=Z(M^\\alpha),\n\\qquad\n\\pi:H\\longrightarrow H/\\Gamma.\n\\tag{Q1}\n$$\n\nAssume the precise compactness hypothesis\n\n<a id=\"equation-q2\"></a>\n$$\nS:=\\pi(\\operatorname{Sp}(\\alpha))\n\\text{ is compact in }H/\\Gamma.\n\\tag{Q2}\n$$\n\nThe whole quotient $H/\\Gamma$ need not be compact.  No separability,\nsigma-finiteness, second-countability, or countable-multiplicity assumption is\nmade.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        }
      ]
    },
    {
      "id": "OA-FLOW.L126.HIST.THICKENINGS",
      "unit": "OA-FLOW-L126",
      "source_file": "src/OA-FLOW-L126.md",
      "source_sha256": "01c4e943b0b161d3febc126f4d6dc380ef2646ead7888cb07c111728ce15635f",
      "reader": "OA-FLOW-L126.html#historical-step-1",
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      "end_line": 358,
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      "prerequisites": [
        "OA-FLOW.CONNES.ABSORPTION",
        "OA-FLOW.CONNES.SUBGROUP",
        "OA-FLOW.L121.SC0",
        "OA-FLOW.GCC.SETTING",
        "OA-FLOW.GCC.INTERSECTION",
        "OA-FLOW.DIRECTED.THICKENING",
        "OA-FLOW.HR.TOPOLOGY"
      ],
      "may_be_used_as_earlier_proved_premise": true,
      "proof_available_after_line": 358,
      "source_level_hypothesis_ranges": [
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 224,
          "end_line": 251,
          "full_statement_context": "Throughout, $G$ is a locally compact Hausdorff abelian group,\n$H=\\widehat G$, $M$ is a nonzero von Neumann algebra, and\n$\\alpha:G\\to\\operatorname{Aut}(M)$ is point-ultraweakly continuous and\ncentrally ergodic.  Put\n\n<a id=\"equation-q1\"></a>\n$$\n\\Gamma=\\Gamma(\\alpha),\n\\qquad\nD=Z(M^\\alpha),\n\\qquad\n\\pi:H\\longrightarrow H/\\Gamma.\n\\tag{Q1}\n$$\n\nAssume the precise compactness hypothesis\n\n<a id=\"equation-q2\"></a>\n$$\nS:=\\pi(\\operatorname{Sp}(\\alpha))\n\\text{ is compact in }H/\\Gamma.\n\\tag{Q2}\n$$\n\nThe whole quotient $H/\\Gamma$ need not be compact.  No separability,\nsigma-finiteness, second-countability, or countable-multiplicity assumption is\nmade.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 252,
          "end_line": 358,
          "full_statement_context": "<a id=\"historical-step-1\"></a>\n### Compact quotient thickenings shrink to the identity coset\n\nFor $0\\ne e\\in\\operatorname{Proj}(D)$, the reduced spectrum absorbs\n$\\Gamma$:\n\n<a id=\"equation-q3\"></a>\n$$\n\\operatorname{Sp}(\\alpha^e)+\\Gamma\n=\\operatorname{Sp}(\\alpha^e).\n\\tag{Q3}\n$$\n\nIndeed, every nonzero fixed projection in $eMe$ is also a nonzero fixed\nprojection in $M$, so\n\n<a id=\"equation-q4\"></a>\n$$\n\\Gamma(\\alpha)\\subseteq\\Gamma(\\alpha^e).\n\\tag{Q4}\n$$\n\nApply the Connes-spectrum absorption law of\n[The dual-center kernel through central overlap](OA-FLOW-L115.md#oa-flow.connes.absorption) to $\\alpha^e$;\n(Q3) follows from (Q4).\n\nLet $U$ range over compact neighborhoods of $0$ in $H$, and set\n\n<a id=\"equation-q5\"></a>\n$$\nA_{e,U}=\\operatorname{Sp}(\\alpha^e)+U,\n\\qquad\nK_{e,U}=\\pi(A_{e,U}).\n\\tag{Q5}\n$$\n\nThe sets $A_{e,U}$ are closed: the sum of a closed set and a compact set is\nclosed in a Hausdorff topological group.  Equation (Q3) makes them\n$\\Gamma$-saturated, so\n\n<a id=\"equation-q6\"></a>\n$$\n\\pi^{-1}(K_{e,U})=A_{e,U}.\n\\tag{Q6}\n$$\n\nThe quotient topology and (Q6) make $K_{e,U}$ closed.  Moreover,\n\n<a id=\"equation-q7\"></a>\n$$\nK_{e,U}\n\\subseteq S+\\pi(U),\n\\tag{Q7}\n$$\n\nand the right side is compact by (Q2).  Hence every $K_{e,U}$ is compact.\n\nThe directed-thickening theorem in\n[Mutual corner approximation through a family of spectral bridges](OA-FLOW-L121.md#oa-flow.directed.thickening)\nshows that the $A_{e,U}$, and therefore the $K_{e,U}$, are downward directed\nunder inclusion.  Restricting to compact neighborhoods loses nothing: inside\nany prescribed neighborhood of zero there is a compact neighborhood small\nenough for the same refinement argument.\n\nTheir intersection is the identity coset.  First,\n$\\Gamma\\subseteq A_{e,U}$ for every pair $(e,U)$.  Conversely, if\n$p\\notin\\Gamma$, the central-corner formula for the Connes spectrum supplies\n$0\\ne e\\in\\operatorname{Proj}(D)$ with\n$p\\notin\\operatorname{Sp}(\\alpha^e)$.  Closedness of that spectrum supplies a\ncompact neighborhood $U$ of zero such that\n\n<a id=\"equation-q8\"></a>\n$$\np\\notin\\operatorname{Sp}(\\alpha^e)+U.\n\\tag{Q8}\n$$\n\nThus\n\n<a id=\"equation-q9\"></a>\n$$\n\\bigcap_{e,U}A_{e,U}=\\Gamma.\n\\tag{Q9}\n$$\n\nBecause every member is saturated, inverse images commute with this\nintersection without losing representatives:\n\n<a id=\"equation-q10\"></a>\n$$\n\\pi^{-1}\\!\\left(\\bigcap_{e,U}K_{e,U}\\right)\n=\\bigcap_{e,U}\\pi^{-1}(K_{e,U})\n=\\Gamma.\n\\tag{Q10}\n$$\n\nConsequently\n\n<a id=\"equation-q11\"></a>\n$$\n\\boxed{\\bigcap_{e,U}K_{e,U}=\\{0+\\Gamma\\}.}\n\\tag{Q11}\n$$\n\nThis saturation step is what justifies passing the infinite intersection to\nthe quotient.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        }
      ]
    },
    {
      "id": "OA-FLOW.L126.HIST.SMALL.CORNER",
      "unit": "OA-FLOW-L126",
      "source_file": "src/OA-FLOW-L126.md",
      "source_sha256": "01c4e943b0b161d3febc126f4d6dc380ef2646ead7888cb07c111728ce15635f",
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      "prerequisites": [
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      "may_be_used_as_earlier_proved_premise": true,
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      "source_level_hypothesis_ranges": [
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 224,
          "end_line": 251,
          "full_statement_context": "Throughout, $G$ is a locally compact Hausdorff abelian group,\n$H=\\widehat G$, $M$ is a nonzero von Neumann algebra, and\n$\\alpha:G\\to\\operatorname{Aut}(M)$ is point-ultraweakly continuous and\ncentrally ergodic.  Put\n\n<a id=\"equation-q1\"></a>\n$$\n\\Gamma=\\Gamma(\\alpha),\n\\qquad\nD=Z(M^\\alpha),\n\\qquad\n\\pi:H\\longrightarrow H/\\Gamma.\n\\tag{Q1}\n$$\n\nAssume the precise compactness hypothesis\n\n<a id=\"equation-q2\"></a>\n$$\nS:=\\pi(\\operatorname{Sp}(\\alpha))\n\\text{ is compact in }H/\\Gamma.\n\\tag{Q2}\n$$\n\nThe whole quotient $H/\\Gamma$ need not be compact.  No separability,\nsigma-finiteness, second-countability, or countable-multiplicity assumption is\nmade.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 359,
          "end_line": 427,
          "full_statement_context": "<a id=\"historical-step-2\"></a>\n### Select a central corner with a small time spectrum\n\nFix\n\n<a id=\"equation-q12\"></a>\n$$\nt\\in\\Gamma^\\perp\n=\\{s\\in G:(s,p)=1\\text{ for every }p\\in\\Gamma\\}.\n\\tag{Q12}\n$$\n\nThe character $p\\mapsto(t,p)$ is constant on cosets of $\\Gamma$, and hence\ndescends to a continuous character $\\chi_t$ of $H/\\Gamma$.  Choose\n\n<a id=\"equation-q12a\"></a>\n$$\n0<\\varepsilon<1-\\frac1{\\sqrt2},\n\\tag{Q12a}\n$$\n\nand define\n\n<a id=\"equation-q13\"></a>\n$$\nO_\\varepsilon\n=\\{q\\in H/\\Gamma:\\operatorname{Re}\\chi_t(q)>1-\\varepsilon\\},\n\\qquad\nU_\\varepsilon=\\pi^{-1}(O_\\varepsilon).\n\\tag{Q13}\n$$\n\nWe use a compact directed-family lemma.  If a downward-directed family of\nnonempty compact sets has intersection contained in an open set $O$, then one\nmember is contained in $O$.  To see this, fix one member $K_0$.  If no member\nlay in $O$, directedness would make the compact sets\n\n<a id=\"equation-q14\"></a>\n$$\nK_0\\cap K\\cap O^c\n\\tag{Q14}\n$$\n\nnonempty with the finite-intersection property.  Their intersection would give\na point in the total intersection outside $O$, a contradiction.\n\nApply this lemma to (Q11) and $O_\\varepsilon$.  For some\n$0\\ne e\\in\\operatorname{Proj}(D)$ and compact neighborhood $U$ of zero,\n\n<a id=\"equation-q15\"></a>\n$$\nK_{e,U}\\subset O_\\varepsilon.\n\\tag{Q15}\n$$\n\nSince $\\operatorname{Sp}(\\alpha^e)\\subset A_{e,U}$, equations\n(Q6), (Q13), and (Q15) give the desired spectral corner:\n\n<a id=\"equation-q16\"></a>\n$$\n\\boxed{\n\\operatorname{Sp}(\\alpha^e)\\subset U_\\varepsilon\n=\\{p\\in H:\\operatorname{Re}(t,p)>1-\\varepsilon\\}.}\n\\tag{Q16}\n$$\n\nOnly compactness of the image $S$ in (Q2) was used to make the quotient\nthickenings compact.\n\n",
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      "id": "OA-FLOW.L126.HIST.GLOBAL.INNERNESS",
      "unit": "OA-FLOW-L126",
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        "OA-FLOW.CONNES.SUBGROUP",
        "OA-FLOW.MINFIX.FULLCONNES",
        "OA-FLOW.PC.2",
        "OA-FLOW.L124.CE5"
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        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 224,
          "end_line": 251,
          "full_statement_context": "Throughout, $G$ is a locally compact Hausdorff abelian group,\n$H=\\widehat G$, $M$ is a nonzero von Neumann algebra, and\n$\\alpha:G\\to\\operatorname{Aut}(M)$ is point-ultraweakly continuous and\ncentrally ergodic.  Put\n\n<a id=\"equation-q1\"></a>\n$$\n\\Gamma=\\Gamma(\\alpha),\n\\qquad\nD=Z(M^\\alpha),\n\\qquad\n\\pi:H\\longrightarrow H/\\Gamma.\n\\tag{Q1}\n$$\n\nAssume the precise compactness hypothesis\n\n<a id=\"equation-q2\"></a>\n$$\nS:=\\pi(\\operatorname{Sp}(\\alpha))\n\\text{ is compact in }H/\\Gamma.\n\\tag{Q2}\n$$\n\nThe whole quotient $H/\\Gamma$ need not be compact.  No separability,\nsigma-finiteness, second-countability, or countable-multiplicity assumption is\nmade.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 428,
          "end_line": 508,
          "full_statement_context": "<a id=\"historical-step-3\"></a>\n### The small cyclic spectrum forces global innerness\n\nSet\n\n<a id=\"equation-q17\"></a>\n$$\n\\sigma=\\alpha_t.\n\\tag{Q17}\n$$\n\nThe projection $e$ in (Q16) is fixed by $\\sigma$.  The individual-operator\nspectrum formula from [The spectrum of one action operator](OA-FLOW-L89.md#oa-flow.opsp.formula),\napplied inside $eMe$, gives\n\n<a id=\"equation-q18\"></a>\n$$\n\\operatorname{Sp}_{\\mathcal L(eMe)}(\\sigma^e)\n=\\overline{\\{(t,p):p\\in\\operatorname{Sp}(\\alpha^e)\\}}.\n\\tag{Q18}\n$$\n\nIt is the action spectrum $\\operatorname{Sp}(\\alpha^e)$ that belongs on the\nright side of (Q18).  Equation (Q16) yields\n\n<a id=\"equation-q19\"></a>\n$$\n\\operatorname{Sp}_{\\mathcal L(eMe)}(\\sigma^e)\n\\subseteq\n\\{z\\in\\mathbb T:\\operatorname{Re}z\\ge1-\\varepsilon\\}.\n\\tag{Q19}\n$$\n\nRegard $\\sigma^e$ as the action of $\\mathbb Z$ on $eMe$.  Its action spectrum\nis the operator spectrum in (Q18), and its Connes spectrum is a subgroup of\n$\\mathbb T$ contained in that spectrum.  The choice (Q12a) has\n$0<\\varepsilon<1$, so the closed arc on the right of (Q19) is contained in a\nproper open semicircle.  No\nnontrivial subgroup of $\\mathbb T$ can be contained in such an arc: the powers\nof any nonidentity element eventually leave it.  Therefore\n\n<a id=\"equation-q20\"></a>\n$$\n\\Gamma(\\sigma^e)=\\{1\\}.\n\\tag{Q20}\n$$\n\nCentral ergodicity makes $e$ full in $M$.  Indeed, its ambient central support\n$z_M(e)$ is a nonzero $\\alpha$-invariant central projection, so\n\n<a id=\"equation-q21\"></a>\n$$\nz_M(e)=1.\n\\tag{Q21}\n$$\n\nThe full fixed-corner theorem from\n[Cancel an inner subgroup, then detect the exact spectrum](OA-FLOW-L119.md#oa-flow.minfix.fullconnes) now\ngives\n\n<a id=\"equation-q22\"></a>\n$$\n\\Gamma(\\sigma)=\\Gamma(\\sigma^e)=\\{1\\}.\n\\tag{Q22}\n$$\n\nEvery $\\alpha_s$ commutes with $\\sigma$ because $G$ is abelian.  Hence\n$\\alpha(G)\\subseteq\\operatorname{Aut}_\\sigma(M)$, and the action of\n$\\operatorname{Aut}_\\sigma(M)$ on $Z(M)$ is ergodic.  Applying the\ncentralizer-ergodicity theorem from\n[Read an inner implementer from a circle eigenunitary](OA-FLOW-L124.md#ce5)\nto (Q22) proves\n\n<a id=\"equation-q23\"></a>\n$$\n\\boxed{\\sigma\\in\\operatorname{Int}(M).}\n\\tag{Q23}\n$$\n\nThe centralizer-ergodicity criterion applies to the whole algebra here.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
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        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 224,
          "end_line": 251,
          "full_statement_context": "Throughout, $G$ is a locally compact Hausdorff abelian group,\n$H=\\widehat G$, $M$ is a nonzero von Neumann algebra, and\n$\\alpha:G\\to\\operatorname{Aut}(M)$ is point-ultraweakly continuous and\ncentrally ergodic.  Put\n\n<a id=\"equation-q1\"></a>\n$$\n\\Gamma=\\Gamma(\\alpha),\n\\qquad\nD=Z(M^\\alpha),\n\\qquad\n\\pi:H\\longrightarrow H/\\Gamma.\n\\tag{Q1}\n$$\n\nAssume the precise compactness hypothesis\n\n<a id=\"equation-q2\"></a>\n$$\nS:=\\pi(\\operatorname{Sp}(\\alpha))\n\\text{ is compact in }H/\\Gamma.\n\\tag{Q2}\n$$\n\nThe whole quotient $H/\\Gamma$ need not be compact.  No separability,\nsigma-finiteness, second-countability, or countable-multiplicity assumption is\nmade.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 509,
          "end_line": 565,
          "full_statement_context": "<a id=\"historical-step-4\"></a>\n### Choose consistent constants and fix the corner implementer\n\nThe tolerance chosen in (Q12a) satisfies\n\n<a id=\"equation-q24\"></a>\n$$\n0<\\varepsilon<1-\\frac1{\\sqrt2}.\n\\tag{Q24}\n$$\n\nPut\n\n<a id=\"equation-q25\"></a>\n$$\n\\theta_0=\\arccos(1-\\varepsilon).\n\\tag{Q25}\n$$\n\nThen $0<\\theta_0<\\pi/4$. Choose a strictly larger open-arc radius\n\n<a id=\"equation-q26\"></a>\n$$\n\\theta_0<\\delta<\\frac\\pi4.\n\\tag{Q26}\n$$\n\nEquations (Q19), (Q25), and (Q26) give\n\n<a id=\"equation-q27\"></a>\n$$\n\\operatorname{Sp}_{\\mathcal L(eMe)}(\\sigma^e)\n\\subseteq\\{e^{ir}:|r|\\le\\theta_0\\}\n\\subset V(\\delta).\n\\tag{Q27}\n$$\n\nThe strict enlargement in (Q26) is needed because (Q19) is a closed spectral\nbound.\n\nBy (Q23), $\\sigma^e$ is inner.  It commutes with the reduced action\n$\\alpha^e$.  The fixed small-spectrum implementer theorem from\n[A central order correction fixes the implementer and retains its bound](OA-FLOW-L125.md#co4),\napplied with the radius $\\delta<\\pi/4$, supplies\n\n<a id=\"equation-q28\"></a>\n$$\nv\\in\\mathcal U((eMe)^{\\alpha^e})\n=\\mathcal U(eM^\\alpha e),\n\\qquad\n\\sigma^e=\\operatorname{Ad}(v).\n\\tag{Q28}\n$$\n\nThus the corner implementer is fixed by the entire reduced action, not merely\nby $\\sigma^e$.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
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    {
      "id": "OA-FLOW.L126.HIST.UNIQUE.LIFT",
      "unit": "OA-FLOW-L126",
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      "proof_available_after_line": 620,
      "source_level_hypothesis_ranges": [
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 224,
          "end_line": 251,
          "full_statement_context": "Throughout, $G$ is a locally compact Hausdorff abelian group,\n$H=\\widehat G$, $M$ is a nonzero von Neumann algebra, and\n$\\alpha:G\\to\\operatorname{Aut}(M)$ is point-ultraweakly continuous and\ncentrally ergodic.  Put\n\n<a id=\"equation-q1\"></a>\n$$\n\\Gamma=\\Gamma(\\alpha),\n\\qquad\nD=Z(M^\\alpha),\n\\qquad\n\\pi:H\\longrightarrow H/\\Gamma.\n\\tag{Q1}\n$$\n\nAssume the precise compactness hypothesis\n\n<a id=\"equation-q2\"></a>\n$$\nS:=\\pi(\\operatorname{Sp}(\\alpha))\n\\text{ is compact in }H/\\Gamma.\n\\tag{Q2}\n$$\n\nThe whole quotient $H/\\Gamma$ need not be compact.  No separability,\nsigma-finiteness, second-countability, or countable-multiplicity assumption is\nmade.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 566,
          "end_line": 620,
          "full_statement_context": "<a id=\"historical-step-5\"></a>\n### Full-corner uniqueness puts the lift in the fixed center\n\nEquations (Q21) and (Q28) meet the hypotheses of the unique inner-lifting\ntheorem from\n[Lifting innerness and cocycles from a full corner](OA-FLOW-L117.md#oa-flow.fullcorner.inner).\nThere is a unique $u\\in\\mathcal U(M)$ such that\n\n<a id=\"equation-q29\"></a>\n$$\n\\sigma=\\operatorname{Ad}(u),\n\\qquad\nue=eu=v.\n\\tag{Q29}\n$$\n\nFor $s\\in G$, the unitary $\\alpha_s(u)$ also implements $\\sigma$, because\n$\\alpha_s$ commutes with $\\sigma$.  Since $e$ and $v$ are fixed,\n\n<a id=\"equation-q30\"></a>\n$$\n\\alpha_s(u)e\n=\\alpha_s(ue)\n=\\alpha_s(v)\n=v.\n\\tag{Q30}\n$$\n\nUniqueness in (Q29) forces\n\n<a id=\"equation-q31\"></a>\n$$\n\\alpha_s(u)=u\n\\qquad(s\\in G),\n\\tag{Q31}\n$$\n\nso $u\\in M^\\alpha$.  Finally, $\\sigma=\\alpha_t$ fixes every element of\n$M^\\alpha$ pointwise.  Equation (Q29) therefore gives\n\n<a id=\"equation-q32\"></a>\n$$\nuxu^*=x\n\\qquad(x\\in M^\\alpha).\n\\tag{Q32}\n$$\n\nTogether, (Q31)–(Q32) show\n\n<a id=\"equation-q33\"></a>\n$$\n\\boxed{u\\in\\mathcal U(Z(M^\\alpha)).}\n\\tag{Q33}\n$$\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        }
      ]
    },
    {
      "id": "OA-FLOW.L126.HIST.ANNIHILATOR",
      "unit": "OA-FLOW-L126",
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        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 224,
          "end_line": 251,
          "full_statement_context": "Throughout, $G$ is a locally compact Hausdorff abelian group,\n$H=\\widehat G$, $M$ is a nonzero von Neumann algebra, and\n$\\alpha:G\\to\\operatorname{Aut}(M)$ is point-ultraweakly continuous and\ncentrally ergodic.  Put\n\n<a id=\"equation-q1\"></a>\n$$\n\\Gamma=\\Gamma(\\alpha),\n\\qquad\nD=Z(M^\\alpha),\n\\qquad\n\\pi:H\\longrightarrow H/\\Gamma.\n\\tag{Q1}\n$$\n\nAssume the precise compactness hypothesis\n\n<a id=\"equation-q2\"></a>\n$$\nS:=\\pi(\\operatorname{Sp}(\\alpha))\n\\text{ is compact in }H/\\Gamma.\n\\tag{Q2}\n$$\n\nThe whole quotient $H/\\Gamma$ need not be compact.  No separability,\nsigma-finiteness, second-countability, or countable-multiplicity assumption is\nmade.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 621,
          "end_line": 660,
          "full_statement_context": "<a id=\"historical-step-6\"></a>\n### Identify the annihilator exactly\n\nWe have proved the difficult inclusion\n\n<a id=\"equation-q34\"></a>\n$$\n\\Gamma^\\perp\n\\subseteq\n\\{s\\in G:\\alpha_s=\\operatorname{Ad}(u)\n\\text{ for some }u\\in\\mathcal U(Z(M^\\alpha))\\}.\n\\tag{Q34}\n$$\n\nFor the reverse inclusion, a central fixed implementer is in particular a\nfixed implementer.  The fixed-implementer annihilator theorem from\n[Small fixed corners, inner spectra and annihilating times](OA-FLOW-L122.md#oa-flow.l122.directannihilator) gives\n\n<a id=\"equation-q35\"></a>\n$$\n\\alpha_s=\\operatorname{Ad}(u),\\quad\nu\\in\\mathcal U(Z(M^\\alpha))\n\\quad\\Longrightarrow\\quad\ns\\in\\Gamma^\\perp.\n\\tag{Q35}\n$$\n\nThis proves Theorem XI.2.9(iii):\n\n<a id=\"equation-q36\"></a>\n$$\n\\boxed{\n\\begin{aligned}\n\\Gamma(\\alpha)^\\perp\n=\\{s\\in G:\\ &\\alpha_s=\\operatorname{Ad}(u)\\\\\n&\\text{for some }u\\in\\mathcal U(Z(M^\\alpha))\\}.\n\\end{aligned}}\n\\tag{Q36}\n$$\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
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      "unit": "OA-FLOW-L126",
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        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 9,
          "end_line": 9,
          "full_statement_context": "Let $M\\ne0$ be a concrete von Neumann algebra on an arbitrary Hilbert space, let $G$ be a locally compact Hausdorff abelian group, and let $\\alpha:G\\to\\operatorname{Aut}(M)$ be a normal point-ultraweakly continuous action. Suppose $Z(M)^\\alpha=\\mathbb C1$. Write $H=\\widehat G$, $F=M^\\alpha$, $D=Z(F)$ and $\\Gamma=\\Gamma(\\alpha)$. Frequencies have the positive L115 convention. For $0<r<\\pi$ put $V(r)=\\{e^{i\\theta}:|\\theta|<r\\}$. An ordinary operator spectrum on a corner is distinguished throughout from the action spectrum in $H$.\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        },
        {
          "source": "src/OA-FLOW-L126.md",
          "start_line": 224,
          "end_line": 251,
          "full_statement_context": "Throughout, $G$ is a locally compact Hausdorff abelian group,\n$H=\\widehat G$, $M$ is a nonzero von Neumann algebra, and\n$\\alpha:G\\to\\operatorname{Aut}(M)$ is point-ultraweakly continuous and\ncentrally ergodic.  Put\n\n<a id=\"equation-q1\"></a>\n$$\n\\Gamma=\\Gamma(\\alpha),\n\\qquad\nD=Z(M^\\alpha),\n\\qquad\n\\pi:H\\longrightarrow H/\\Gamma.\n\\tag{Q1}\n$$\n\nAssume the precise compactness hypothesis\n\n<a id=\"equation-q2\"></a>\n$$\nS:=\\pi(\\operatorname{Sp}(\\alpha))\n\\text{ is compact in }H/\\Gamma.\n\\tag{Q2}\n$$\n\nThe whole quotient $H/\\Gamma$ need not be compact.  No separability,\nsigma-finiteness, second-countability, or countable-multiplicity assumption is\nmade.\n\n",
          "usage": "Full hypotheses and statement context; not a separate proved premise."
        }
      ]
    },
    {
      "id": "OA-FLOW.L126.HIST.SOLVED.PROBLEM",
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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          "full_statement_context": "<a id=\"l129-setting\"></a>\n<a id=\"oa-flow.l129.setting\"></a>\n## Setting and earlier proofs\n\nThroughout, finite groups act by normal star automorphisms on nonzero concrete von Neumann algebras of arbitrary Hilbert dimension. An action is **free** if, for every nonidentity group element $s$, the relation $cx=\\alpha_s(x)c$ for every $x$ forces $c=0$. A **unitary cocycle** is a family $u_s\\in\\mathcal U(M)$ satisfying $u_{st}=u_s\\alpha_s(u_t)$ and $u_e=1$. We impose no separability or countable-decomposability hypothesis. Sums of nonnegative numbers mean suprema of finite subsums; orthogonal operator sums mean strong limits of finite sums.\n\nThe regular crossed-product coefficients, their uniqueness, the faithful normal completely positive identity-coefficient expectation, and the free relative commutant are proved in [Discrete Fourier columns, finite corners and orbit MASAs](OA-FLOW-L128.md#l128-fc0), FC0–FC4. Its [regular-model transport theorem](OA-FLOW-L128.md#regular-transport) identifies the model in every faithful normal representation. [Projection comparison and the countably decomposable type III case](OA-FLOW-PC.md#oa-flow.pc.0), PC0–PC7, supplies projection joins, polar decomposition, central supports, comparison, Cantor–Bernstein, full-corner centers, finite joins, proper infiniteness and the exact faithful-normal-state criterion for countable decomposability. The cardinal tools are HF1–HF2, LC2–LC3 and CA1 of [Transport a fixed corner, then assemble its local cardinal](OA-FLOW-L120.md#oa-flow.l120.central-cardinal-partition). Those local projection lemmas apply to arbitrary algebras, without the action hypotheses used elsewhere in that lesson.\n\nThe trace input is the general finite-algebra theorem in [The normalized trace with its full center retained](OA-FLOW-FCT.md#oa-flow.fct.6), FCT6–FCT8. The trace Hilbert space and its representation are constructed in [Finite ideals and GNS spaces for arbitrary weights](OA-FLOW-GW.md#oa-flow.gw.3), GW3–GW4; their normality follows from [Order-normal positive functionals and ultraweak continuity](OA-FLOW-NF.md#oa-flow.nf.5), NF5, and the faithful normal inverse and ultrastrong topology are proved in [Concrete predual balls and faithful ultraweak representations](OA-FLOW-ST12.md#oa-flow.st.2), ST2. Normal functional supports use NF1, and the normality criterion for positive functionals uses NF1–NF4. The standard-form alternative uses [All projection corners and canonical positive-functional vectors](OA-FLOW-CR.md#oa-flow.cr.9), CR9 and its natural-cone construction, [Canonical standard-form transport and finite balanced matrix cones](OA-FLOW-MC.md#oa-flow.mc.1), MC1, and [A normal regular construction on arbitrary Hilbert spaces](OA-FLOW-NR.md#oa-flow.nr.1), NR1. A finite discrete group automatically satisfies the continuity hypotheses of NR1.\n\n"
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