Near-optimal small-depth lower bounds for small distance connectivity

TL;DR

This paper establishes near-optimal lower bounds on the size of small-depth circuits for small distance connectivity, advancing understanding of circuit complexity for this fundamental graph problem.

Contribution

It introduces a new lower bound technique using random projections and applies it to prove tight bounds for small-depth circuit complexity of small distance connectivity.

Findings

Lower bounds close to optimal for small-depth circuits solving small distance connectivity

Introduction of random projections as a new technique in circuit lower bounds

Demonstration that improving bounds further would imply major complexity class separations

Abstract

We show that any depth-$d$ circuit for determining whether an $n$-node graph has an $s$-to-$t$ path of length at most $k$ must have size $n^{\Omega(k^{1/d}/d)}$. The previous best circuit size lower bounds for this problem were $n^{k^{\exp(-O(d))}}$ (due to Beame, Impagliazzo, and Pitassi [BIP98]) and $n^{\Omega((\log k)/d)}$ (following from a recent formula size lower bound of Rossman [Ros14]). Our lower bound is quite close to optimal, since a simple construction gives depth-$d$ circuits of size $n^{O(k^{2/d})}$ for this problem (and strengthening our bound even to $n^{k^{\Omega(1/d)}}$ would require proving that undirected connectivity is not in $\mathsf{NC^1}.$) Our proof is by reduction to a new lower bound on the size of small-depth circuits computing a skewed variant of the "Sipser functions" that have played an important role in classical circuit lower bounds [Sip83, Yao85, H{\aa}s86]. A key ingredient in our proof of the required lower bound for these Sipser-like functions is the use of \emph{random projections}, an extension of random restrictions which were recently employed in [RST15]. Random projections allow us to obtain sharper quantitative bounds while employing simpler arguments, both conceptually and technically, than in the previous works [Ajt89, BPU92, BIP98, Ros14].