Coboundary and cosystolic expansion without dependence on dimension or degree

Yotam Dikstein, Irit Dinur
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引用次数: 4

Abstract

We give new bounds on the cosystolic expansion constants of several families of high dimensional expanders, and the known coboundary expansion constants of order complexes of homogeneous geometric lattices, including the spherical building of $SL_n(F_q)$. The improvement applies to the high dimensional expanders constructed by Lubotzky, Samuels and Vishne, and by Kaufman and Oppenheim. Our new expansion constants do not depend on the degree of the complex nor on its dimension, nor on the group of coefficients. This implies improved bounds on Gromov's topological overlap constant, and on Dinur and Meshulam's cover stability, which may have applications for agreement testing. In comparison, existing bounds decay exponentially with the ambient dimension (for spherical buildings) and in addition decay linearly with the degree (for all known bounded-degree high dimensional expanders). Our results are based on several new techniques: * We develop a new"color-restriction"technique which enables proving dimension-free expansion by restricting a multi-partite complex to small random subsets of its color classes. * We give a new"spectral"proof for Evra and Kaufman's local-to-global theorem, deriving better bounds and getting rid of the dependence on the degree. This theorem bounds the cosystolic expansion of a complex using coboundary expansion and spectral expansion of the links. * We derive absolute bounds on the coboundary expansion of the spherical building (and any order complex of a homogeneous geometric lattice) by constructing a novel family of very short cones.
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给出了几种高维展开子族的协缩展开常数的新界,以及齐次几何格阶复形的已知协缩展开常数,包括球面构造$SL_n(F_q)$。这种改进适用于由Lubotzky, Samuels和Vishne以及Kaufman和Oppenheim构建的高维扩展器。我们新的膨胀常数不依赖于复合体的程度,也不依赖于它的维数,也不依赖于系数群。这意味着改进了Gromov拓扑重叠常数和Dinur和Meshulam覆盖稳定性的界,可以应用于一致性检验。相比之下,现有的边界随环境尺寸呈指数衰减(对于球形建筑物),并且随度线性衰减(对于所有已知的有界度高维扩展器)。我们的结果基于几种新技术:*我们开发了一种新的“颜色限制”技术,通过将多部复合体限制为其颜色类的小随机子集来证明无维展开。*对Evra和Kaufman的局部到全局定理给出了新的“谱”证明,得到了更好的界,摆脱了对度的依赖。这个定理用连杆的共边界展开和谱展开限定了复合体的协收缩展开。*我们通过构造一组新颖的极短锥,推导了球面建筑(以及齐次几何晶格的任何阶复合体)共边界展开的绝对界。
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