==== TABLE OF CONTENTS ==== Counterexamples-to-the-duality-conjecture-for-metric-entropy//01-introduction.tex Counterexamples-to-the-duality-conjecture-for-metric-entropy//02-matrix-contract.tex Counterexamples-to-the-duality-conjecture-for-metric-entropy//03-compression.tex Counterexamples-to-the-duality-conjecture-for-metric-entropy//04-partitions.tex Counterexamples-to-the-duality-conjecture-for-metric-entropy//05-counterexample.tex Counterexamples-to-the-duality-conjecture-for-metric-entropy//paper.tex Counterexamples-to-the-duality-conjecture-for-metric-entropy//pivot-comparison.tex Counterexamples-to-the-duality-conjecture-for-metric-entropy//preamble.tex Counterexamples-to-the-duality-conjecture-for-metric-entropy//references.bib =========================== ==== BEGIN Counterexamples-to-the-duality-conjecture-for-metric-entropy//01-introduction.tex ==== \section{Introduction}\label{sec:introduction} For bounded sets $A,B$ in a finite-dimensional real vector space, with $B$ having nonempty interior, let $N(A,B)$ denote the least number of translates of $B$ that cover $A$. The translation vectors may lie anywhere in the ambient space. For an origin-symmetric convex body $K\subset\R^n$, its polar is \[ K^\circ=\{y\in\R^n:\langle x,y\rangle\le1 \text{ for every }x\in K\}. \] Here a convex body is compact and has nonempty interior. All logarithms are natural. The duality conjecture for metric entropy, originating in Pietsch's operator-theoretic work in 1972, asks whether there are absolute constants $a,b\ge1$ such that \begin{equation}\label{eq:duality-conjecture} \frac1b\log N(L^\circ,aK^\circ) \le \log N(K,L) \le b\log N(L^\circ,a^{-1}K^\circ) \end{equation} for every dimension and every pair of origin-symmetric convex bodies $K,L$; see \cite[Conjecture~1]{AMSTJ2004}. It asks whether passing to the polar pair preserves covering complexity up to universal changes of scale and multiplicative constants. We disprove the full conjecture. \begin{theorem}\label{thm:main} For every $a,b\ge1$, there are a positive integer $n$ and an origin-symmetric convex body $K\subset\R^n$ such that, with $L=[-1,1]^n$, \[ \log N(K,L)>b\log N(L^\circ,a^{-1}K^\circ). \] \end{theorem} Thus the upper bound in \eqref{eq:duality-conjecture} fails for every proposed pair of absolute constants. In particular, the two-sided duality conjecture has a negative answer. The bodies in Theorem~\ref{thm:main} have nonempty interior in the full ambient dimension. Their dimensions grow with the parameters; no assertion about a fixed dimension is intended. \subsection{Related work} The question developed from the duality problem for entropy numbers of operators; Artstein, Milman and Szarek give the geometric and operator formulations in \cite[pp.~1314--1315]{AMS2004} and attribute the original problem to Pietsch's 1972 work. Early progress already showed that polarity controls covering numbers in several regimes. K\"onig and Milman proved a comparison of the $n$th roots of the two covering numbers \cite[Theorem~1]{KonigMilman1987}; on the logarithmic scale this allows an additive error proportional to $n$. Bourgain, Pajor, Szarek and Tomczak-Jaegermann established entropy-number comparisons under geometric and sequence-regularity assumptions, as well as estimates with losses depending on the rank \cite{BPSTJ1989}. Artstein, Milman and Szarek proved the dimension-free conjecture when one body is a Euclidean ball, and hence when either body is an ellipsoid \cite[Theorem~1]{AMS2004}. Artstein, Milman, Szarek and Tomczak-Jaegermann proved universal duality for \emph{convexified packing} \cite[Theorem~2]{AMSTJ2004}. This quantity uses an ordered sequence of points: the interior of the translate centered at each new point must avoid the convex hull of its predecessors. That requirement is stronger than pairwise separation and differs from the ordinary covering number in \eqref{eq:duality-conjecture}. They also announced ordinary entropy duality for spaces whose K-convexity constant is bounded, with the comparison constants depending on that bound \cite[Theorem~5]{AMSTJ2004}; see also the later derivation in \cite[Section~2]{Milman2007}. A bound for each individual finite-dimensional space does not provide one pair of constants for all spaces and dimensions. For arbitrary symmetric convex bodies, Emanuel Milman obtained a comparison with logarithmic losses in both the scale and the entropy factor \cite[Corollary~1.2]{Milman2007}. Connections with learning theory provide another perspective: Hu, Peale and Reingold study dual covering numbers of function classes, obtaining a comparison with an explicit prefactor depending on the approximation scale and the uniform bounds of the function classes \cite[Theorem~11]{HuPealeReingold2022}. These dimension- or scale-dependent estimates are compatible with the failure of a universal pair $a,b$. The column approximation in this paper also belongs to the broader study of entropy of convex hulls. For example, Mendelson develops finite-set convex-hull estimates in $L_2(\mu)$ using Maurey's approximation method \cite[Section~2.1]{Mendelson2001}. Here the approximation is uniform over all row coordinates and uses the special partition structure: labels replace the original centers in the finite encoding. The finite-field side uses the polynomial zero estimate associated with Schwartz and Zippel \cite{Schwartz1980,Zippel1979}, together with diagonal recovery of symmetric multilinear forms in sufficiently large characteristic \cite{FerreroMicali1979,DrapalVojtechovsky2009}. We prove the precise elementary forms of these tools and the additional compression and separation arguments below. Theorem~\ref{thm:main} also separates ordinary covering entropy from convexified-packing entropy, even after a fixed change of scale; Corollary~\ref{cor:convexified-separation} states and proves this consequence after the construction. \subsection{The construction and its main mechanism} The proof starts with a finite real matrix whose entries lie in $[0,1]$. Its rows are pairwise separated by one in the sup norm, while the absolutely convex hull of its columns admits a small uniform approximation list. A direct support-function calculation converts these two properties into large primal entropy and small polar entropy. The approximation statement is the reusable part of the argument. Suppose a finite set carries $u$ partitions, each with at most $q$ classes. For a subset $T$ of the partition indices, join two points whenever they belong to the same class in one partition indexed by $T$. We consider the resulting graph distances $d_T$, allowing infinite distance between components. For a positive integer cutoff $h$, define the profiles \[ x\longmapsto \max\left\{0,1-\frac{\log(1+d_T(x,v))}{\log(1+h)}\right\}, \] with value zero at infinite distance. The columns consist of these profiles over all centers $v$ and over a family of sets $T$, each omitting only a small fraction of the partitions. Proposition~\ref{prop:compression} gives a uniform approximation of every nonnegative combination of these columns whose coefficients sum to at most one. For a given combination, averaging finds one partition present in all but a small amount of coefficient mass. At each distance level, a greedy selection of a bounded number of pivots captures all but a small residual mass at every point. Each pivot can then be replaced by a fixed representative of its class in the common partition. This replacement requires storing a label, rather than a point of the original set. The replacement enlarges the relevant distance radii from $j$ to at most $3j+2$. The logarithmic profile bounds the error caused by this enlargement by $\log3/\log(1+h)$, uniformly over all columns and all graph components. After grouping weights by pivot slot and by $T$, the approximation count depends on $q$ through a fixed power. It does not depend on the number of possible column centers through an additional factor. Both the choice of the common partition and all grouped weights are included in the count. Splitting a signed coefficient vector into its positive and negative parts then gives an approximation list for the absolutely convex column hull, with twice the full error of the nonnegative approximation and the square of the list size. To obtain separated rows, we use symmetric $h$-linear forms on $\F_p^r$, where $p$ is a sufficiently large prime and $r$ is a positive integer. A probabilistic choice of directions ensures that, for every nonzero form, one can delete a small fraction of the directions so that no evaluation on a remaining $h$-tuple vanishes, including tuples with repetitions. Contraction with one direction supplies a partition. A short path in the associated graph would express a nonzero form as a sum of forms killed by the directions along the path, contradicting the nonvanishing property. There are $p^{D_h}$ rows but at most $p^{D_{h-1}}$ labels in each partition, where $D_j=\binom{r+j-1}{j}$ for $j\ge0$. The ratio \[ \frac{D_{h-1}}{D_h}=\frac{h}{r+h-1} \] tends to zero as $r$ grows with $h$ fixed. All remaining encoding costs are fixed before the prime $p$ is chosen. Taking $p$ sufficiently large therefore makes those costs negligible. This order of choices is what allows the compression result and the separation construction to produce a failure of dimension-free entropy duality. Section~\ref{sec:convex-bodies} first proves the matrix-to-body conversion, which serves as the construction target. Section~\ref{sec:compression} then establishes uniform compression for an arbitrary admissible family of partitions. Section~\ref{sec:partitions} constructs the finite-field partitions and proves row separation. Finally, Section~\ref{sec:parameters} chooses the parameters and applies the conversion to defeat any proposed universal constants, then derives the convexified-packing consequence. All arguments needed for the construction are included. \subsection{Notation} For a finite set $S$, write \[ B_\infty^S=[-1,1]^S,\qquad B_1^S=\left\{\lambda\in\R^S: \sum_{s\in S}|\lambda_s|\le1\right\}. \] The sup norm on functions on $S$ is denoted by $\|\cdot\|_{\infty,S}$. For a finite collection of vectors, $\absconv$ denotes the convex hull of the vectors and their negatives. A uniform $\varepsilon$-approximation list may have centers outside the class being approximated; actual centers in the coefficient ball will be chosen in Lemma~\ref{lem:matrix-to-bodies}. We write $[u]=\{1,\ldots,u\}$. ==== END Counterexamples-to-the-duality-conjecture-for-metric-entropy//01-introduction.tex ==== ==== BEGIN Counterexamples-to-the-duality-conjecture-for-metric-entropy//02-matrix-contract.tex ==== \section{The matrix construction target} \label{sec:convex-bodies} The geometric part of the argument is an elementary conversion of a real matrix into a pair of convex bodies. It specifies exactly what the two combinatorial constructions must achieve: many separated rows and a small uniform approximation list for the absolutely convex hull of the columns. The small cube added to the row hull ensures nonempty interior without losing the polar covering estimate. \begin{lemma}[Matrix-to-body conversion] \label{lem:matrix-to-bodies} Let $X$ and $Y$ be finite nonempty sets, and let $g_y\colon X\to\R$, $y\in Y$, be real functions. Write \[ R_x=(g_y(x))_{y\in Y}\in\R^Y, \qquad f_\lambda=\sum_{y\in Y}\lambda_y g_y, \qquad \mathcal F=\{f_\lambda:\|\lambda\|_1\le1\}. \] Suppose that \[ \|R_x-R_{x'}\|_\infty\ge1 \quad\text{for all distinct }x,x'\in X, \] and that, for some $\varepsilon>0$, there is a list of $M$ functions on $X$ such that every member of $\mathcal F$ is within $\varepsilon$ of a function on the list in the uniform norm. The functions on the list need not belong to $\mathcal F$. For $t>0$, set \[ K=3\absconv\{R_x:x\in X\}+tB_\infty^Y, \qquad L=B_\infty^Y. \] Then $K,L$ are origin-symmetric compact convex bodies with nonempty interior in $\R^Y$, and \begin{equation} \label{eq:matrix-body-bounds} N(K,L)\ge |X|, \qquad N\bigl(L^\circ,(6\varepsilon+2t)K^\circ\bigr)\le M. \end{equation} Both covering numbers use arbitrary ambient translation centers. \end{lemma} \begin{proof} The hull $\absconv\{R_x:x\in X\}$ is the convex hull of the finitely many vectors $\pm R_x$. It is compact, convex, and symmetric, and contains zero. Thus $K$ has the same three properties and contains $tB_\infty^Y$, which gives it nonempty interior in the full ambient space. The corresponding properties of $L$ are immediate. Each point $3R_x$ belongs to $K$, and two distinct such points have uniform distance at least $3$. Every translate of $L$ has uniform diameter $2$, whatever its center. Hence it contains at most one of these $|X|$ points. This proves the first inequality in \eqref{eq:matrix-body-bounds}. For the polar estimate, the support function $h_K(\delta)=\sup_{z\in K}\langle z,\delta\rangle$ is exactly \begin{equation} \label{eq:row-support-function} h_K(\delta) =3\max_{x\in X}|\langle R_x,\delta\rangle| +t\sum_{y\in Y}|\delta_y| =3\|f_\delta\|_{\infty,X}+t\|\delta\|_1. \end{equation} Indeed, a linear functional attains its maximum over the finite convex hull at one of the vectors $\pm R_x$. Its maximum over $B_\infty^Y$ is $\sum_y|\delta_y|$, attained by choosing the sign of each coordinate. The two choices in the Minkowski sum are independent, so their maxima add. The same cube calculation gives \[ L^\circ=B_1^Y=\{\lambda\in\R^Y:\|\lambda\|_1\le1\}. \] Order the approximating list. Assign each $\lambda\in B_1^Y$ to the first list function within $\varepsilon$ of $f_\lambda$, thereby partitioning $B_1^Y$ into at most $M$ nonempty clusters. From each nonempty cluster choose one actual vector $\lambda^{(k)}\in B_1^Y$. For any $\lambda$ in that cluster, the triangle inequality gives \[ \|f_\lambda-f_{\lambda^{(k)}}\|_{\infty,X} \le2\varepsilon, \qquad \|\lambda-\lambda^{(k)}\|_1\le2. \] Consequently \eqref{eq:row-support-function} implies \[ h_K(\lambda-\lambda^{(k)})\le6\varepsilon+2t. \] For every $c>0$, the definition of the polar and positive homogeneity give the equivalence \[ \delta\in cK^\circ \quad\Longleftrightarrow\quad h_K(\delta)\le c. \] Each cluster is therefore contained in $\lambda^{(k)}+(6\varepsilon+2t)K^\circ$. These at most $M$ translates cover $B_1^Y=L^\circ$, proving the second inequality. Selecting representatives inside the coefficient ball is what controls the contribution of the added cube, even when the original list functions lie outside $\mathcal F$. \end{proof} For proposed constants $a,b\ge1$, the lemma reduces the problem to finding a matrix and positive numbers $\varepsilon,t$ for which \[ \log|X|>b\log M, \qquad 6\varepsilon+2t\le a^{-1}. \] Indeed, increasing the polar covering body preserves the cover supplied by the lemma. The next two sections construct the matrix. The compression argument controls $M$ through the number of labels in a partition; the finite-field construction makes that number small relative to the row count on the logarithmic scale. ==== END Counterexamples-to-the-duality-conjecture-for-metric-entropy//02-matrix-contract.tex ==== ==== BEGIN Counterexamples-to-the-duality-conjecture-for-metric-entropy//03-compression.tex ==== \section{Uniform compression from partitions} \label{sec:compression} We first prove an approximation result for an arbitrary family of partitions of a finite set. Its cost depends on the number of labels of a partition, whereas the underlying set can be much larger. Let $X$ be a finite nonempty set, let $u,q$ be positive integers, and let \[ L_i:X\longrightarrow\Sigma_i,\qquad i\in[u]=\{1,\ldots,u\}, \qquad |L_i(X)|\le q. \] Fix $0<\theta<1$ and a nonempty family $\mathcal T$ of subsets of $[u]$ such that \begin{equation} |[u]\setminus T|\le\theta u\qquad(T\in\mathcal T). \label{eq:admissible-sets} \end{equation} In particular, every $T\in\mathcal T$ is nonempty. For each such $T$, form the undirected graph on $X$ in which distinct vertices $x,z$ are adjacent when $L_i(x)=L_i(z)$ for some $i\in T$. Write $d_T(x,z)$ for its graph distance, with distance $\infty$ between different components. Choose a positive integer $h$ such that \begin{equation} \frac{\log3}{\log(h+1)}\le\theta, \qquad s=\lceil1/\theta\rceil. \label{eq:compression-parameters} \end{equation} Define the logarithmic profile \[ \phi_h(d)=\max\left\{0,1-\frac{\log(d+1)}{\log(h+1)}\right\} \quad(d=0,1,2,\ldots),\qquad \phi_h(\infty)=0. \] Set $Y=X\times\mathcal T$. For $y=(v,T)\in Y$, define the column function \begin{equation} g_y(x)=\phi_h(d_T(x,v))\qquad(x\in X). \label{eq:column-functions} \end{equation} Thus $0\le g_y\le1$. For nonnegative coefficients of total mass at most one, write \[ f_\mu=\sum_{y\in Y}\mu_y g_y, \qquad \mathcal F_+=\left\{f_\mu:\mu_y\ge0,\ \sum_{y\in Y}\mu_y\le1\right\}. \] For a function $f:X\to\R$, let $\|f\|_{\infty,X}=\max_{x\in X}|f(x)|$. We seek a uniform approximation list for $\mathcal F_+$ whose size is controlled by $h,\theta,u,q$, rather than $|X|$. The next lemma expresses each profile as a weighted sum of graph-ball indicators and bounds the error caused by enlarging their radii from $j$ to $3j+2$. \begin{lemma}[Logarithmic profile] \label{lem:log-profile} For any positive integer $h$, the weights \[ \gamma_j=\frac{\log(j+2)-\log(j+1)}{\log(h+1)} \quad(0\le j\max\{h,h^2u^{2h}\}. \label{eq:field-prime-threshold} \end{equation} There exist $t_1,\ldots,t_u\in E=\F_p^r$ such that, for every nonzero $Z\in\operatorname{Sym}^h(E^*)$, there is a set $T\subseteq[u]$ with $|[u]\setminus T|\le\theta u$ for which \begin{equation} Z(t_{i_1},\ldots,t_{i_h})\ne0 \qquad\text{for all }(i_1,\ldots,i_h)\in T^h. \label{eq:robust-nonvanishing} \end{equation} Tuples in this assertion may have repeated indices. \end{proposition} \begin{proof} Choose $t_1,\ldots,t_u$ independently and uniformly in $E$. Fix a nonzero form $Z$. For $z=\sum_{a=1}^r z_a e_a$, its diagonal polynomial is \begin{equation} \begin{aligned} P_Z(z_1,\ldots,z_r)&=Z(z,\ldots,z)\\ &=\sum_{\substack{\alpha_1+\cdots+\alpha_r=h\\\alpha_a\ge0}} \frac{h!}{\alpha_1!\cdots\alpha_r!} Z(e_1^{[\alpha_1]},\ldots,e_r^{[\alpha_r]}) z_1^{\alpha_1}\cdots z_r^{\alpha_r}, \end{aligned} \label{eq:diagonal-polynomial} \end{equation} where $e_a^{[\alpha_a]}$ means that $e_a$ is repeated $\alpha_a$ times among the arguments. At least one displayed value of $Z$ is nonzero. Since $p>h$, every displayed multinomial coefficient is nonzero in $\F_p$. Distinct multisets give distinct monomials, so $P_Z$ is a nonzero polynomial of total degree $h$. This is the diagonal recovery of a symmetric multilinear form when $h!$ is invertible; see \cite[Corollary~1.2]{FerreroMicali1979} and \cite[Proposition~3.3]{DrapalVojtechovsky2009}. The coordinate argument above gives the precise fact needed here. For an ordered tuple $\mathbf i=(i_1,\ldots,i_h)\in[u]^h$, let $\supp(\mathbf i)=\{i_1,\ldots,i_h\}$. The expression $Z(t_{i_1},\ldots,t_{i_h})$, considered as a polynomial in the scalar coordinates of the vectors with indices in $\supp(\mathbf i)$, has total degree $h$ and is nonzero: setting all those vector variables equal to $z$ gives the nonzero polynomial \eqref{eq:diagonal-polynomial}. Lemma~\ref{lem:polynomial-zero} therefore gives \begin{equation} \Pr\bigl(Z(t_{i_1},\ldots,t_{i_h})=0\bigr)\le\frac hp. \label{eq:tuple-zero-probability} \end{equation} This applies to every pattern of repeated indices. For this fixed $Z$, evaluations on tuples with pairwise disjoint index supports depend on disjoint subsets of the independent vectors $t_i$. Their zero events are consequently independent. There are at most $u^{hw}$ ordered lists of $w$ ordered $h$-tuples, and fewer than $p^{D_h}$ choices of nonzero $Z$. A union bound shows that the probability that some nonzero $Z$ has $w$ zero tuples with pairwise disjoint supports is at most \begin{equation} p^{D_h}u^{hw}\left(\frac hp\right)^w =\left(\frac{h^2u^{2h}}p\right)^{D_h}<1. \label{eq:field-union-bound} \end{equation} The count includes all forms over the chosen field; no independence between different forms is needed. Fix vectors for which this event does not occur. For each nonzero $Z$, take a family of zero tuples with pairwise disjoint supports that is maximal under inclusion. It contains at most $w-1$ tuples. Delete the union of their supports, and let $T$ be the remaining indices. The number deleted is at most \[ h(w-1)h. \label{eq:graph-separation} \end{equation} Consequently, for $Y=X\times\mathcal T$ and $R_x=(g_{(v,T)}(x))_{(v,T)\in Y}\in\R^Y$, the rows satisfy \begin{equation} \|R_x-R_y\|_\infty=1\qquad(x\ne y). \label{eq:row-separation} \end{equation} \end{proposition} \begin{proof} The cardinality of $X$ follows from \eqref{eq:symmetric-form-dimension}. The contraction $L_i(x)$ is a symmetric $(h-1)$-linear form, so its possible values belong to a space of cardinality $p^{D_{h-1}}$. This bounds the realized labels even if a contraction is not surjective. Fix distinct $x,y\in X$, and apply Proposition~\ref{prop:robust-directions} to $Z=y-x$. Let $T\in\mathcal T$ be the resulting nonempty set. Recall that distinct vertices are adjacent in the graph for $T$ if their labels agree at some $i\in T$. Suppose there were a path \[ x=x_0,x_1,\ldots,x_k=y,\qquad 1\le k\le h. \] For each edge choose $i_j\in T$ such that $L_{i_j}(x_j)=L_{i_j}(x_{j-1})$, and put $\Delta_j=x_j-x_{j-1}$. Thus \[ \Delta_j(t_{i_j},v_2,\ldots,v_h)=0 \qquad\text{for every }v_2,\ldots,v_h\in E. \] Choose any $i_*\in T$, and form the $h$-tuple consisting of $t_{i_1},\ldots,t_{i_k}$ followed by $h-k$ copies of $t_{i_*}$. Every $\Delta_j$ vanishes on this tuple, since it is symmetric and one of its arguments is $t_{i_j}$. The identity $Z=\sum_{j=1}^k\Delta_j$ implies that $Z$ also vanishes on the tuple, contrary to \eqref{eq:robust-nonvanishing}. This proves \eqref{eq:graph-separation}; vertices in different components have infinite distance and already satisfy it. At the column $(x,T)$, the logarithmic profile gives $g_{(x,T)}(x)=1$ and $g_{(x,T)}(y)=0$, because $d_T(x,y)>h$. All column values lie in $[0,1]$, so this unit difference also gives the exact equality \eqref{eq:row-separation}. \end{proof} The family $\mathcal T$ here contains every admissible subset and is fixed with the partitions. The separating set $T$ may depend on the pair of rows. This is compatible with Proposition~\ref{prop:compression}, whose common index may depend on the particular convex combination of columns. If $h$ also satisfies $\log3/\log(h+1)\le\theta$, the compression bound applies with $q=p^{D_{h-1}}$ and $s=\lceil1/\theta\rceil$, giving \begin{equation} \log Q\le hsD_{h-1}\log p+C_{h,\theta,u}. \label{eq:field-compression-bound} \end{equation} Once $r,h,\theta$ are fixed, so are $u$ and $C_{h,\theta,u}$; the prime $p$ can still be taken arbitrarily large subject to \eqref{eq:field-prime-threshold}. ==== END Counterexamples-to-the-duality-conjecture-for-metric-entropy//04-partitions.tex ==== ==== BEGIN Counterexamples-to-the-duality-conjecture-for-metric-entropy//05-counterexample.tex ==== \section{Choice of parameters and failure of duality} \label{sec:parameters} We now choose the parameters in their order of dependence. The field size is chosen last, so it can absorb the encoding term from Proposition~\ref{prop:compression}. \begin{proof}[Proof of Theorem~\ref{thm:main}] Fix $a,b\ge1$. Put \[ \theta=\frac1{1000a}, \qquad s=\lceil1/\theta\rceil, \] and choose a positive integer $h$ with $\log3/\log(h+1)\le\theta$. Such an integer exists because $\log(h+1)$ tends to infinity. Choose a positive integer $r$ so that \begin{equation} \label{eq:rank-choice} r+h-1>8bh^2s. \end{equation} As in Section~\ref{sec:partitions}, define \[ D_j=\binom{r+j-1}{j}\quad(0\le j\le h), \qquad w=2D_h, \qquad u=\left\lceil\frac{hw}{\theta}\right\rceil. \] The number \begin{equation} \label{eq:fixed-encoding-term} C=C_{h,\theta,u} =\log u+hs2^u\log\left(1+\frac{s2^u}{\theta}\right) \end{equation} is now fixed. Choose a prime $p$ satisfying \begin{equation} \label{eq:prime-choice} p>\max\left\{ h,\ h^2u^{2h},\ \exp\left(\frac{8bC}{D_h}\right) \right\}. \end{equation} All quantities on the right have already been determined, and primes exceed every finite bound. Apply Proposition~\ref{prop:robust-directions} with these parameters, and form the label maps and graph profiles in Proposition~\ref{prop:separated-rows}. The row index set $X$ consists of the symmetric $h$-linear forms on $\F_p^r$, so \[ m=|X|=p^{D_h}>1. \] Each label map takes at most $q=p^{D_{h-1}}$ values. The columns are indexed by $Y=X\times\mathcal T$, where \[ \mathcal T=\{T\subseteq[u]:|[u]\setminus T|\le\theta u\}, \] and the real row vectors satisfy \begin{equation} \label{eq:final-row-separation} \|R_x-R_{x'}\|_\infty=1\qquad(x\ne x'). \end{equation} In particular, $Y$ is a finite nonempty set. The finite field serves only to construct the indices and label maps; the matrix entries and the convex bodies below are real. By Proposition~\ref{prop:compression}, the positive column class has a uniform $3\theta$ approximation list of cardinality $Q$ satisfying \[ \log Q\le hs\log q+C =hsD_{h-1}\log p+C. \] Corollary~\ref{cor:signed-compression} gives a uniform $6\theta$ approximation list of at most $Q^2$ functions for the absolutely convex column hull. Thus Lemma~\ref{lem:matrix-to-bodies} applies with $\varepsilon=6\theta$ and $t=\theta$. It gives admissible bodies in dimension $n=|Y|$, \begin{equation} \label{eq:final-bodies} K=3\absconv\{R_x:x\in X\}+\theta B_\infty^Y, \qquad L=B_\infty^Y, \end{equation} such that \[ N(K,L)\ge m, \qquad N(L^\circ,38\theta K^\circ)\le Q^2. \] Since $38\theta=38/(1000a)1$ gives \[ b\log N(L^\circ,a^{-1}K^\circ) \le b\log(Q^2) <\frac12\log m <\log N(K,L). \] Identifying $\R^Y$ with $\R^n$ makes $L=[-1,1]^n$ and proves the claimed counterexample for the arbitrary proposed constants $a,b$. \end{proof} The same estimate gives an asymptotic form of the conclusion. Fix $a\ge1$, and hence $\theta,h,s$. For each positive integer $r$, set $D_h,u,C$ as above and choose a prime \[ p>\max\left\{h,\ h^2u^{2h},\ \exp\left(\frac{rC}{D_h}\right) \right\}. \] The resulting bodies $K_r,L_r$ satisfy \[ 0\le \frac{\log N(L_r^\circ,a^{-1}K_r^\circ)} {\log N(K_r,L_r)} \le \frac{2h^2s}{r+h-1}+\frac2r \longrightarrow0. \] Although $u$ and $C$ may grow rapidly with $r$, both are fixed before $p$ is chosen. No upper bound on the resulting ambient dimension is required for this conclusion. \subsection{A consequence for convexified packing} Theorem~\ref{thm:main} also separates ordinary covering entropy from convexified-packing entropy. For a nonempty bounded set $T$ and an origin-symmetric convex body $B$, let $\widehat M(T,B)$ be the largest length of an ordered sequence $x_1,\ldots,x_m\in T$ such that \[ (x_j+\operatorname{int}B)\cap\conv\{x_i:iC\log\widehat M(K,L/A). \] \end{corollary} \begin{proof} An ordered $B$-convexly separated sequence has at most one point in each translate of $B/4$: two such points have difference in $B/2\subset\operatorname{int}B$, contradicting the separation condition. Consequently $\widehat M(T,B)\le N(T,B/4)$, with no boundary ambiguity for covers by closed translates. The universal convexified duality bound \cite[Theorem~2]{AMSTJ2004}, applied to $K,L/A$, gives \[ \begin{split} \widehat M(K,L/A) &\le\widehat M(A L^\circ,K^\circ/2)^2\\ &=\widehat M(L^\circ,K^\circ/(2A))^2\\ &\le N(L^\circ,K^\circ/(8A))^2. \end{split} \] Here the equality uses simultaneous dilation of both arguments. Choose $K,L$ by Theorem~\ref{thm:main} with $a=8A$ and $b=2C$. Taking logarithms in the displayed bound proves the corollary. \end{proof} ==== END Counterexamples-to-the-duality-conjecture-for-metric-entropy//05-counterexample.tex ==== ==== BEGIN Counterexamples-to-the-duality-conjecture-for-metric-entropy//paper.tex ==== \documentclass[11pt]{article} \usepackage{cmap} \input{preamble} \title{Counterexamples to the duality conjecture\\for metric entropy} \author{OpenAI} \date{September 24, 2026} \begin{document} \maketitle \begin{abstract} We disprove Pietsch's dimension-free duality conjecture for metric entropy. For every proposed pair of universal constants, we construct origin-symmetric convex bodies that violate the corresponding covering-entropy inequality, already when the covering body is a cube. \end{abstract} \input{sections/01-introduction} \input{sections/02-matrix-contract} \input{sections/03-compression} \input{sections/04-partitions} \input{sections/05-counterexample} \bibliographystyle{alpha} \begingroup \raggedright \bibliography{references} \endgroup \end{document} ==== END Counterexamples-to-the-duality-conjecture-for-metric-entropy//paper.tex ==== ==== BEGIN Counterexamples-to-the-duality-conjecture-for-metric-entropy//pivot-comparison.tex ==== \begin{figure}[hbp] \centering \begin{minipage}[t]{.48\linewidth} \centering {\small\textup{(a)} Keeping an assigned match\par} \medskip \begin{tikzpicture}[font=\small, point/.style={circle,fill=black,inner sep=1.6pt}, path/.style={draw=black!75,line width=.6pt}, bound/.style={draw=linkblue,dashed,line width=.7pt}] \node[point,label=above:$x$] (x) at (0,0) {}; \node[point,label=above:$v$] (v) at (1.5,0) {}; \node[point,label=above:$z$] (z) at (3,0) {}; \node[point,label=above:$z'$] (zp) at (4.5,0) {}; \draw[path] (x) -- node[below] {$\le j$} (v); \draw[path] (v) -- node[below] {$\le j$} (z); \draw[path] (z) -- node[below] {$\le1$} (zp); \draw[bound] (x) to[bend right=40] node[below=3pt,text=linkblue] {$d_T(x,z')\le2j+1$} (zp); \path (0,-1.55) -- (4.5,-1.55); \end{tikzpicture} \end{minipage}\hfill \begin{minipage}[t]{.48\linewidth} \centering {\small\textup{(b)} Controlling the extra matches\par} \medskip \begin{tikzpicture}[font=\small, point/.style={circle,fill=black,inner sep=1.6pt}, path/.style={draw=black!75,line width=.6pt}, bound/.style={draw=linkblue,dashed,line width=.7pt}] \node[point,label=above:$x$] (x) at (0,0) {}; \node[point,label=above:$z'$] (zp) at (3.8,0) {}; \node[point,label=below:$v$] (v) at (3.8,-1.2) {}; \draw[path] (x) -- node[above] {$\le2j+1$} (zp); \draw[path] (zp) -- node[right] {$\le j+1$} (v); \draw[bound] (x) -- node[below left,text=linkblue] {$\le3j+2$} (v); \path (0,-1.55) -- (4.5,-1.55); \end{tikzpicture} \end{minipage} \caption{The two triangle inequalities in the compression step. The pivot $z$ is replaced by its fixed label representative $z'$. The diagrams show schematic graph paths; the labels are upper bounds on their lengths. The logarithmic profile controls the enlargement to radius $3j+2$.} \label{fig:pivot-comparison} \end{figure} ==== END Counterexamples-to-the-duality-conjecture-for-metric-entropy//pivot-comparison.tex ==== ==== BEGIN Counterexamples-to-the-duality-conjecture-for-metric-entropy//preamble.tex ==== \usepackage[T1]{fontenc} \usepackage{lmodern} \usepackage[margin=1in]{geometry} \usepackage{amsmath,amssymb,amsthm,mathtools} \usepackage{microtype} \usepackage{enumitem} \usepackage{xcolor} \usepackage{tikz} \usetikzlibrary{arrows.meta,calc} \definecolor{linkblue}{RGB}{24,62,110} \usepackage[colorlinks=true,linkcolor=linkblue,citecolor=linkblue,urlcolor=linkblue,bookmarksnumbered=true]{hyperref} \hypersetup{pdftitle={Counterexamples to the duality conjecture for metric entropy},pdfauthor={OpenAI}} \newtheorem{theorem}{Theorem}[section] \newtheorem{proposition}[theorem]{Proposition} \newtheorem{lemma}[theorem]{Lemma} \newtheorem{corollary}[theorem]{Corollary} \theoremstyle{definition} \newtheorem{definition}[theorem]{Definition} \newtheorem{remark}[theorem]{Remark} \newcommand{\R}{\mathbb R} \newcommand{\N}{\mathbb N} \newcommand{\F}{\mathbb F} \DeclareMathOperator{\absconv}{absconv} \DeclareMathOperator{\supp}{supp} \DeclareMathOperator{\dist}{dist} \DeclareMathOperator{\im}{im} \DeclareMathOperator{\Sym}{Sym} \DeclareMathOperator{\conv}{conv} \DeclareMathOperator{\diam}{diam} \DeclareMathOperator{\rank}{rank} \setlist[enumerate]{label=\textup{(\roman*)},leftmargin=*,itemsep=.25em} \setlist[itemize]{leftmargin=*,itemsep=.25em} \setlength{\emergencystretch}{1.5em} \numberwithin{equation}{section} \ifdefined\pdfinfoomitdate\pdfinfoomitdate=1\fi \ifdefined\pdftrailerid\pdftrailerid{}\fi \ifdefined\pdfsuppressptexinfo\pdfsuppressptexinfo=15\fi ==== END Counterexamples-to-the-duality-conjecture-for-metric-entropy//preamble.tex ==== ==== BEGIN Counterexamples-to-the-duality-conjecture-for-metric-entropy//references.bib ==== @article{AMS2004, author = {Artstein, S. and Milman, V. and Szarek, S. 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