Correlation Bounds Against Monotone NC^1

Benjamin Rossman
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引用次数: 14

Abstract

This paper gives the first correlation bounds under product distributions, including the uniform distribution, against the class mNC1 of polynomial-size O(log n)-depth monotone circuits. Our main theorem, proved using the pathset complexity framework introduced in [56], shows that the average-case k-CYCLE problem (on Erdos-Renyi random graphs with an appropriate edge density) is [EQUATION] hard for mNC1. Combining this result with O'Donnell's hardness amplification theorem [43], we obtain an explicit monotone function of n variables (in the class mSAC1) which is [EQUATION] hard for mNC1 under the uniform distribution for any desired constant e > 0. This bound is nearly best possible, since every monotone function has agreement [EQUATION] with some function in mNC1 [44]. Our correlation bounds against mNC1 extend smoothly to non-monotone NC1 circuits with a bounded number of negation gates. Using Holley's monotone coupling theorem [30], we prove the following lemma: with respect to any product distribution, if a balanced monotone function f is [EQUATION] hard for monotone circuits of a given size and depth, then f is [EQUATION] hard for (non-monotone) circuits of the same size and depth with at most t negation gates. We thus achieve a lower bound against NC1 circuits with [EQUATION] log n negation gates, improving the previous record of 1/6 log log n [7]. Our bound on negations is "half" optimal, since ⌈log(n + 1)⌉ negation gates are known to be fully powerful for NC1 [3, 21].
单调NC^1的相关界
本文给出了多项式大小为O(log n)深度单调电路的mNC1类在乘积分布(包括均匀分布)下的第一相关界。我们的主要定理,使用[56]中引入的路径集复杂度框架证明,表明平均情况下k-CYCLE问题(在具有适当边密度的Erdos-Renyi随机图上)对于mNC1是[EQUATION]困难的。结合这一结果与O'Donnell的硬度放大定理[43],我们得到了n个变量(在mSAC1类中)的显式单调函数,在任意期望常数e > 0的均匀分布下,该函数对于mSAC1是[EQUATION] hard。这个界几乎是最好的可能,因为每个单调函数都与mNC1[44]中的某些函数一致[EQUATION]。我们对mNC1的相关界限平滑地扩展到具有有限数量的负栅极的非单调NC1电路。利用Holley的单调耦合定理[30],我们证明了以下引理:对于任何积分布,如果一个平衡单调函数f对于给定大小和深度的单调电路是[EQUATION]困难的,那么对于相同大小和深度的(非单调)电路来说f是[EQUATION]困难的,并且最多有t个负闸。因此,我们通过[EQUATION] log n个负门实现了针对NC1电路的下界,改进了之前1/6 log log n的记录[7]。我们的否定界是“半”最优的,因为已知对于NC1而言,≤log(n + 1)²的否定门是完全有效的[3,21]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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