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Cuts, the cubic map and a quartic potential

Written by Claude Opus 5.5 (Anthropic), October 2026. Self-checked by the writing AI. Public domain (CC0).

This lesson prepares the two tools of the proof that \(\ell_1\) has metric Markov cotype two. The first tool replaces finitely many points of \(\ell_1\) by vertices of a cube \([0,1]^{\mathcal B}\) with weighted coordinates, in such a way that the distance in \(\ell_1\) becomes the square of a Hilbert distance, and gives a map from the whole cube back into \(\ell_1\) that does not increase distances. The second tool is an inequality for the map \(\Phi\) of the cube that applies the cubic \(\phi(r)=3r^2-2r^3\) to every coordinate. The squared change of \(\Phi\) between two points of the cube is bounded by the change of the fourth power of the Hilbert distance to a vertex, up to a term that is linear in the displacement. For a random displacement with mean zero the linear term disappears.

The lesson follows [OpenAI-MC, Sections 2 and 3]. It uses only finite sums, absolutely convergent series and the Cauchy–Schwarz inequality. The definitions of Metric Markov cotype two are not needed here.

1. Cuts

The space \(\ell_1\) consists of the real sequences \(x=(x(k))_{k\ge1}\) with \(\|x\|_1=\sum_k|x(k)|<\infty\). Let \(x_1,\dots,x_n\in\ell_1\) with \(n\ge2\). A cut is a subset \(B\) of \([n]=\{1,\dots,n\}\) that is neither empty nor all of \([n]\). Write \(r_+=\max\{r,0\}\). For a cut \(B\) and a coordinate \(k\) put \[ b_B(k)=\Bigl(\min_{i\in B}x_i(k)-\max_{i\notin B}x_i(k)\Bigr)_+ , \] and put \(v(k)=\min_ix_i(k)\). So \(b_B(k)>0\) exactly if in the coordinate \(k\) all points with index in \(B\) lie strictly above all other points, and then \(b_B(k)\) is the gap between the two groups.

The sequences \(v\) and \(b_B\) lie in \(\ell_1\): \(|v(k)|\le\sum_i|x_i(k)|\), and for \(i_0\in B\) and \(j_0\notin B\), \[ 0\le b_B(k)\le|x_{i_0}(k)|+|x_{j_0}(k)| . \] The weight of a cut is \(w_B=\|b_B\|_1\). Let \(\mathcal B\) be the set of the cuts with \(w_B>0\). It has at most \(2^n-2\) elements.

Lemma 1.1 (one coordinate). Fix \(k\), and let \(\alpha_1<\alpha_2<\dots<\alpha_m\) be the different values among \(x_1(k),\dots,x_n(k)\). For \(1\le r<m\) let \[ B_r=\{\,i:\ x_i(k)\ge\alpha_{r+1}\,\} . \] Then \(B_r\) is a cut with \(b_{B_r}(k)=\alpha_{r+1}-\alpha_r\), and \(b_B(k)=0\) for every other cut \(B\).

Proof. The set \(B_r\) contains an index with the value \(\alpha_m\) and no index with the value \(\alpha_1\), so it is a cut. The smallest value on \(B_r\) is \(\alpha_{r+1}\) and the largest value outside is \(\alpha_r\). Conversely let \(b_B(k)>0\), and let \(\alpha_{r+1}\) be the smallest value on \(B\) and \(\alpha'\) the largest value outside \(B\); then \(\alpha'<\alpha_{r+1}\). Every index with a value \(\ge\alpha_{r+1}\) lies in \(B\), because its value exceeds \(\alpha'\); every index in \(B\) has a value \(\ge\alpha_{r+1}\). So \(B=\{i:x_i(k)\ge\alpha_{r+1}\}\), and \(r\ge1\) because \(B\) is not all of \([n]\). \(\blacksquare\)

So in one coordinate the cuts that matter are nested: \(B_1\supset B_2\supset\dots\supset B_{m-1}\). The index \(i\) lies in \(B_r\) exactly if \(\alpha_{r+1}\le x_i(k)\).

Let \(z_i\in\{0,1\}^{\mathcal B}\) be the vector that records which cuts contain \(i\): \[ z_i(B)=\begin{cases}1&\text{if }i\in B,\\0&\text{if }i\notin B.\end{cases} \] Define the map \(T\) from \(\mathbb R^{\mathcal B}\) to \(\ell_1\) by \[ T(u)=v+\sum_{B\in\mathcal B}u_B\,b_B . \] It is affine, and its values lie in \(\ell_1\) because the sum is finite.

Proposition 1.2 (cut representation). Let \(x_1,\dots,x_n\in\ell_1\). If the points are not all equal, then \(\mathcal B\) is not empty, and for all \(i,j\in[n]\) and all \(u,u'\in\mathbb R^{\mathcal B}\), with sums over \(B\in\mathcal B\): \[ \begin{gathered} T(z_i)=x_i,\\ \|x_i-x_j\|_1=\sum_Bw_B\,|z_i(B)-z_j(B)|,\\ \|T(u)-T(u')\|_1\le\sum_Bw_B\,|u_B-u'_B| . \end{gathered} \] The second equation also holds with \((z_i(B)-z_j(B))^2\) in place of the absolute value. The three statements are called parts 1, 2 and 3.

Proof. Cuts outside \(\mathcal B\) have \(b_B=0\), so in every coordinate sums over \(\mathcal B\) of terms with a factor \(b_B(k)\) can be taken over all cuts. Fix \(k\) and use the notation of Lemma 1.1.

Part 1. By Lemma 1.1, \[ T(z_i)(k)=\alpha_1+\sum_{r:\ i\in B_r}(\alpha_{r+1}-\alpha_r) . \] The index \(i\) lies in \(B_r\) exactly if \(\alpha_{r+1}\le x_i(k)\). So the sum runs over the gaps below \(x_i(k)\), and their total is \(x_i(k)-\alpha_1\).

Part 2. Let \(x_i(k)\ge x_j(k)\). No cut \(B_r\) contains \(j\) without containing \(i\), and \(B_r\) contains \(i\) without \(j\) exactly if \(x_j(k)<\alpha_{r+1}\le x_i(k)\). The gaps of these \(r\) add up to \(x_i(k)-x_j(k)\). So \[ \begin{aligned} &|x_i(k)-x_j(k)|\\ &\qquad=\sum_B|z_i(B)-z_j(B)|\,b_B(k) , \end{aligned} \] and the same holds if \(x_i(k)<x_j(k)\), by symmetry. Sum over \(k\); the sum over the finitely many \(B\) can be exchanged with the sum over \(k\), and \(\sum_kb_B(k)=w_B\). The numbers \(z_i(B)-z_j(B)\) are \(0\) or \(\pm1\), so their absolute values are their squares.

If \(\mathcal B\) were empty, part 2 would give \(\|x_i-x_j\|_1=0\) for all \(i,j\). So \(\mathcal B\) is not empty if the points are not all equal.

Part 3. \(T(u)-T(u')=\sum_B(u_B-u'_B)\,b_B\), and \(\|b_B\|_1=w_B\). \(\blacksquare\)

Example 1.3. Let \(x_1=(0,0)\), \(x_2=(1,0)\), \(x_3=(1,2)\) (all further coordinates \(0\)). In the first coordinate the values are \(0<1\), with the cut \(\{2,3\}\) and the gap \(1\). In the second coordinate the values are \(0<2\), with the cut \(\{3\}\) and the gap \(2\). So \(\mathcal B=\{\{2,3\},\{3\}\}\) with the weights \(1\) and \(2\), \(v=0\), \(b_{\{2,3\}}=(1,0)\), \(b_{\{3\}}=(0,2)\), and \[ z_1=(0,0),\quad z_2=(1,0),\quad z_3=(1,1) . \] For instance \(\|x_1-x_3\|_1=3=1\cdot1+2\cdot1\).

Example 1.4 (the map \(T\) leaves the span of the points). Let \(x_1,x_2,x_3\) be the first three unit vectors of \(\ell_1\). In the coordinate \(k\le3\) the values are \(0<1\), with the cut \(\{k\}\) and the gap \(1\). So \(\mathcal B=\{\{1\},\{2\},\{3\}\}\) with weights \(1\), \(v=0\), and \(T(u)=(u_1,u_2,u_3,0,0,\dots)\). The points \(x_i\) lie in the plane of the vectors with coordinate sum \(1\), but \(T\) maps the cube onto the cube \([0,1]^3\). For instance \(T(0)=0\) is the coordinatewise median of the three points. The new points of the cotype inequality will be of the form \(T(u)\), and this is where they can leave a subspace that contains the old points.

2. The cube and the cubic map

From here to the end of the lesson \(\mathcal B\) is any finite nonempty set and \((w_B)_{B\in\mathcal B}\) are positive numbers. On \(\mathbb R^{\mathcal B}\) use the norm \[ \|u\|_{1,w}=\sum_Bw_B\,|u_B| \] and the inner product and norm \[ \begin{gathered} \langle u,u'\rangle_H=\sum_Bw_B\,u_Bu'_B,\\ \|u\|_H=\sqrt{\langle u,u\rangle_H} . \end{gathered} \] Write \(H\) for \(\mathbb R^{\mathcal B}\) with this inner product. The Cauchy–Schwarz inequality gives, for \(a,\delta\in\mathbb R^{\mathcal B}\), \[ \sum_Bw_B\,|a_B|\,|\delta_B|\le\|a\|_H\,\|\delta\|_H . \] Let \(Q=[0,1]^{\mathcal B}\) be the cube. Its vertices are the vectors in \(\{0,1\}^{\mathcal B}\). For two vertices \(e,e'\) the differences \(e_B-e'_B\) are \(0\) or \(\pm1\), so \[ \|e-e'\|_{1,w}=\|e-e'\|_H^2 . \] With the weights and vertices \(z_i\) of Proposition 1.2 this reads \[ \|x_i-x_j\|_1=\|z_i-z_j\|_{1,w}=\|z_i-z_j\|_H^2 . \] So the squared distances in \(\ell_1\), which occur in the cotype inequality, are fourth powers of distances in \(H\). Part 3 of Proposition 1.2 says that \(T\) does not increase distances from \(\|\cdot\|_{1,w}\) to \(\|\cdot\|_1\).

Definition. Let \(\phi(r)=3r^2-2r^3\) for \(0\le r\le1\), and let \(\Phi\) be the map of \(Q\) that applies \(\phi\) to every coordinate: \(\Phi(u)_B=\phi(u_B)\).

Lemma 2.1. 1. \(\phi'(r)=6r(1-r)\). The function \(\phi\) is increasing on \([0,1]\) with \(\phi(0)=0\) and \(\phi(1)=1\). So \(\Phi\) maps \(Q\) into \(Q\) and fixes every vertex.

  1. For \(r\in[0,1]\) and \(d\in\{0,1\}\): \(|\phi'(r)|\le6\,|r-d|\).

  2. \(\phi(r)=r^3+3r^2(1-r)\), and \(\phi(1-r)=1-\phi(r)\).

Proof. 1 is a computation. 2: \(6r(1-r)\le6r\) and \(6r(1-r)\le6(1-r)\). 3: \(r^3+3r^2-3r^3=\phi(r)\); and \(\phi(r)+\phi(1-r)\) is the sum of the four terms \(r^3\), \(3r^2(1-r)\), \(3r(1-r)^2\), \((1-r)^3\) of the expansion of \((r+(1-r))^3=1\). \(\blacksquare\)

Part 3 has a reading in terms of chance: if three independent events have the probability \(r\) each, then \(\phi(r)\) is the probability that at least two of them occur. Part 2 is the property that matters: the derivative of \(\phi\) vanishes at both ends of the interval, to first order. The map \(\Phi\) is flat at the vertices of the cube.

3. The flat inequality

Fix a vertex \(e\) of the cube. For \(u\in Q\) put \[ F_e(u)=\|u-e\|_H^4 . \]

Lemma 3.1 (increments of \(\Phi\)). Let \(u,u'\in Q\), and put \(a=u-e\) and \(\delta=u'-u\). Then \[ \begin{aligned} &\|\Phi(u')-\Phi(u)\|_{1,w}\\ &\qquad\le6\,\|a\|_H\|\delta\|_H+3\,\|\delta\|_H^2 . \end{aligned} \]

Proof. Fix \(B\). The points \(u_B+\sigma\delta_B\), \(0\le\sigma\le1\), lie in \([0,1]\), and \[ \begin{aligned} &\phi(u'_B)-\phi(u_B)\\ &\qquad=\delta_B\int_0^1\phi'(u_B+\sigma\delta_B)\,d\sigma . \end{aligned} \] By Lemma 2.1 with \(d=e_B\), \[ \begin{aligned} |\phi'(u_B+\sigma\delta_B)|&\le6\,|u_B+\sigma\delta_B-e_B|\\ &\le6\,|a_B|+6\sigma\,|\delta_B| . \end{aligned} \] Integrating over \(\sigma\) gives \[ |\phi(u'_B)-\phi(u_B)|\le6\,|a_B|\,|\delta_B|+3\,\delta_B^2 . \] Multiply by \(w_B\), sum over \(B\), and use the Cauchy–Schwarz inequality for the first term. \(\blacksquare\)

Lemma 3.2 (the remainder of the fourth power). For \(a,\delta\in H\) let \[ R=\|a+\delta\|_H^4-\|a\|_H^4-4\,\|a\|_H^2\langle a,\delta\rangle_H . \] Then \[ R=2\,\|a\|_H^2\|\delta\|_H^2+\bigl(2\langle a,\delta\rangle_H+\|\delta\|_H^2\bigr)^2 . \] In particular \(R\ge0\), \(\|a\|_H^2\|\delta\|_H^2\le\tfrac12R\) and \(\|\delta\|_H^4\le4R\).

Proof. Write \(\alpha=\|a\|_H^2\) and \(\gamma=2\langle a,\delta\rangle_H+\|\delta\|_H^2\), so that \(\|a+\delta\|_H^2=\alpha+\gamma\). Then \[ \begin{aligned} R&=(\alpha+\gamma)^2-\alpha^2-4\alpha\langle a,\delta\rangle_H\\ &=2\alpha\bigl(\gamma-2\langle a,\delta\rangle_H\bigr)+\gamma^2\\ &=2\alpha\,\|\delta\|_H^2+\gamma^2 . \end{aligned} \] Both terms are \(\ge0\), which gives the first two consequences. For the third, \(\|\delta\|_H^2=\gamma-2\langle a,\delta\rangle_H\), so \[ \begin{aligned} \|\delta\|_H^4&\le2\gamma^2+8\langle a,\delta\rangle_H^2\\ &\le2\gamma^2+8\,\alpha\,\|\delta\|_H^2\\ &\le4R . \end{aligned} \] \(\blacksquare\)

The term \(4\|a\|_H^2\langle a,\delta\rangle_H\) is the derivative of \(a\mapsto\|a\|_H^4\) in the direction \(\delta\). So \(R\) is the error of the linear approximation of the fourth power, and the lemma bounds it from below.

Proposition 3.3 (the flat inequality). Let \(u,u'\in Q\) and let \(e\) be a vertex of \(Q\). With \(a=u-e\) and \(\delta=u'-u\), \[ \begin{aligned} &\|\Phi(u')-\Phi(u)\|_{1,w}^2\\ &\quad\le108\,\bigl(F_e(u')-F_e(u)\\ &\qquad\qquad-4\,\|a\|_H^2\langle a,\delta\rangle_H\bigr) . \end{aligned} \]

Proof. The expression in the bracket is the number \(R\) of Lemma 3.2, because \(u'-e=a+\delta\). Square the inequality of Lemma 3.1 and use \((\alpha+\beta)^2\le2\alpha^2+2\beta^2\): \[ \begin{aligned} &\|\Phi(u')-\Phi(u)\|_{1,w}^2\\ &\qquad\le72\,\|a\|_H^2\|\delta\|_H^2+18\,\|\delta\|_H^4\\ &\qquad\le36R+72R . \end{aligned} \] \(\blacksquare\)

4. Displacements with mean zero

Corollary 4.1. Let \(u\in Q\) and let \(e\) be a vertex of \(Q\). Let \(u^1,\dots,u^m\in Q\) and \(\rho_1,\dots,\rho_m\ge0\) with \(\sum_l\rho_l=1\) and \[ \sum_l\rho_l\,u^l=u . \] Then \[ \begin{aligned} &\sum_l\rho_l\,\|\Phi(u^l)-\Phi(u)\|_{1,w}^2\\ &\qquad\le108\,\Bigl(\sum_l\rho_l\,F_e(u^l)-F_e(u)\Bigr) . \end{aligned} \]

Proof. Apply Proposition 3.3 to \(u\) and \(u^l\), with \(\delta^l=u^l-u\), multiply by \(\rho_l\) and sum. The linear terms add up to \(4\|a\|_H^2\langle a,\sum_l\rho_l\delta^l\rangle_H=0\). \(\blacksquare\)

In words: let a random point of the cube have the mean \(u\). Then the mean squared distance, in the norm \(\|\cdot\|_{1,w}\), between the images under \(\Phi\) of the random point and of its mean is at most \(108\) times the mean increase of the potential \(F_e\). The vertex \(e\) is arbitrary. In the next lesson the corollary is applied to every step of a walk, and the increases of the potential add up to a telescoping sum.

Example 4.2 (the identity map does not satisfy such an inequality). Take one coordinate with the weight \(1\), the vertex \(e=0\), a number \(0<\varepsilon\le\tfrac12\), the point \(u=\varepsilon\) and the two points \(u^1=0\), \(u^2=2\varepsilon\) with \(\rho_1=\rho_2=\tfrac12\). The potential is \(F_0(u)=u^4\), and \[ \begin{aligned} \sum_l\rho_lF_0(u^l)-F_0(u)&=\tfrac12(2\varepsilon)^4-\varepsilon^4\\ &=7\varepsilon^4 . \end{aligned} \] Without the map \(\Phi\), the mean squared distance of the two points from \(u\) is \(\varepsilon^2\), which is not bounded by a constant times \(\varepsilon^4\). With the map: \(\phi(\varepsilon)-\phi(0)=3\varepsilon^2-2\varepsilon^3\) and \(\phi(2\varepsilon)-\phi(\varepsilon)=9\varepsilon^2-14\varepsilon^3\), so the mean squared distance of the images is at most \(\tfrac12(9+81)\varepsilon^4=45\varepsilon^4\). Near a vertex the potential is of the fourth order, and a map of the cube can obey the inequality only if its changes are of the second order there. This is the reason for the cubic: \(\phi'\) vanishes at \(0\) and at \(1\).

5. Exercises

5.1. Compute \(\mathcal B\), the weights, \(v\) and the vectors \(z_i\) for \(x_1=(0,3)\), \(x_2=(2,1)\), \(x_3=(5,1)\), and check part 2 of Proposition 1.2 for the three pairs.

5.2. In the setting of Section 1 show that \(\sum_Bb_B(k)=\max_ix_i(k)-\min_ix_i(k)\) for every \(k\), and conclude that for \(u\in Q\) every coordinate of \(T(u)\) lies between the smallest and the largest value of the points in this coordinate.

5.3. Let \(n=3\) and let \(\mu\in\{0,1\}^{\mathcal B}\) be the vertex with \(\mu_B=1\) exactly if \(B\) has at least two elements. Show that \(T(\mu)\) is the coordinatewise median of \(x_1,x_2,x_3\).

5.4. Show that \(\|\Phi(u')-\Phi(u)\|_{1,w}\le\tfrac32\,\|u'-u\|_{1,w}\) for \(u,u'\in Q\), and that the constant \(\tfrac32\) cannot be replaced by a smaller one.

5.5. Take one coordinate with the weight \(w\), the vertex \(e=0\), the point \(u=\tfrac12\) and the two points \(\tfrac12\pm\eta\) with probabilities \(\tfrac12\), where \(0<\eta\le\tfrac12\). Compute both sides of Corollary 4.1.

6. Solutions

5.1. First coordinate: the values are \(0<2<5\), with the cuts \(\{2,3\}\) (gap \(2\)) and \(\{3\}\) (gap \(3\)). Second coordinate: the values are \(1<3\), with the cut \(\{1\}\) (gap \(2\)). So \(\mathcal B=\{\{2,3\},\{3\},\{1\}\}\) with the weights \(2,3,2\), and \(v=(0,1)\). In this order of the cuts, \(z_1=(0,0,1)\), \(z_2=(1,0,0)\), \(z_3=(1,1,0)\). Distances: \(\|x_1-x_2\|_1=4=2+2\); \(\|x_1-x_3\|_1=7=2+3+2\); \(\|x_2-x_3\|_1=3\).

5.2. By Lemma 1.1 the sum is \(\sum_{r=1}^{m-1}(\alpha_{r+1}-\alpha_r)=\alpha_m-\alpha_1\). For \(u\in Q\), \(T(u)(k)=v(k)+\sum_Bu_Bb_B(k)\) with \(0\le u_B\le1\) and \(b_B(k)\ge0\), so \(\alpha_1\le T(u)(k)\le\alpha_1+(\alpha_m-\alpha_1)\).

5.3. Fix \(k\). By Lemma 1.1, \(T(\mu)(k)\) is \(\alpha_1\) plus the gaps \(\alpha_{r+1}-\alpha_r\) of those \(r\) for which \(B_r\) has at least two elements, that is, for which at least two of the three points have a value \(\ge\alpha_{r+1}\) in the coordinate \(k\). This holds exactly if the median of the three values is \(\ge\alpha_{r+1}\). So the sum of these gaps is the median minus \(\alpha_1\).

5.4. \(\phi'(r)=6r(1-r)\) has the largest value \(\tfrac32\) on \([0,1]\), at \(r=\tfrac12\). So \(|\phi(r')-\phi(r)|\le\tfrac32|r'-r|\) for \(r,r'\in[0,1]\); multiply by \(w_B\) and sum. For one coordinate and \(u=\tfrac12\), \(u'=\tfrac12+\eta\), the quotient of the two sides is \(\tfrac32-2\eta^2\) (see the next solution), which tends to \(\tfrac32\) as \(\eta\to0\).

5.5. \(\phi(\tfrac12\pm\eta)=\tfrac12\pm(\tfrac32\eta-2\eta^3)\), and \(\|\cdot\|_{1,w}\) is \(w\) times the absolute value. So the left side is \(w^2(\tfrac32\eta-2\eta^3)^2\). The potential is \(F_0(u)=(wu^2)^2\), and \[ \begin{aligned} &\tfrac12\bigl(\tfrac12+\eta\bigr)^4+\tfrac12\bigl(\tfrac12-\eta\bigr)^4-\tfrac1{16}\\ &\qquad=\tfrac32\eta^2+\eta^4 . \end{aligned} \] So the right side is \(108\,w^2(\tfrac32\eta^2+\eta^4)\). The left side is at most \(\tfrac94w^2\eta^2\), so in this example the inequality holds with \(\tfrac32\) in place of \(108\).

References