An improved lower bound on the Banach--Mazur distance to the cross-polytope
Omer Friedland
TL;DR
The work establishes a sharper lower bound on the Banach--Mazur distance from the Gaussian Gluskin polytope to the cross-polytope in the regime $m=n^3$, showing $d_{\rm BM}(G_m,B_1^n) \ge c n^{4/7}(\log n)^{-C}$ w.h.p. by combining a discretization/powering framework with a novel treatment of many small coefficients via Maurey sparsification and a thickening-stable Gaussian measure bound. The analysis splits into a small-$U$ regime, handled via random suppression and Gram--Schmidt control, and a large-$U$ regime, addressed through sparsification inside a quotient space and union bounds. A careful balance of entropy reduction and small-ball estimates yields the $4/7$ exponent, advancing the understanding of optimal distortion to the cross-polytope and moving closer to the known upper bound $n^{5/6}$. The results have implications for the geometry of random quotients of $\ell_1^m$ and related probabilistic nets in high dimensions.
Abstract
Let $Γ$ be an $n\times m$ matrix with independent standard Gaussian entries and let $G_m = Γ(B_1^m)$ be the associated Gaussian Gluskin polytope (equivalently, a random $n$-dimensional quotient of $\ell_1^m$). In the regime $m = n^3$ we prove that, with probability at least $1-2/n$, $$ d_{\mathrm{BM}}(G_m,B_1^n) \ge c n^{4/7}(\log n)^{-C}, $$ where $B_1^n = \conv\{\pm e_1,\dots,\pm e_n\}$ is the cross-polytope. This improves the previously best-known exponent $5/9$ (up to logarithmic factors) for this Gaussian model; in particular, the same lower bound holds for $\sup_{K} d_{\mathrm{BM}}(K,B_1^n)$. The main new ingredient is a conditioning-compatible treatment of the regime of ``many small-coefficients''. After passing to a suitable Gaussian quotient, we apply a Maurey-type sparsification that reduces the relevant entropy (in effect shrinking the support size from $k$ to $k/\log(nρ)$) at the cost of a Euclidean thickening. We control this enlargement via a Gaussian measure bound stable under Euclidean thickening. In the complementary regime of ``few small-coefficients'', we give a streamlined argument avoiding the global tilting step in earlier work. Together these ingredients rebalance entropy and small-ball estimates and yield the exponent $4/7$.
