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Super-Linear Gate and Super-Quadratic Wire Lower Bounds for Depth-Two and Depth-Three Threshold Circuits

24 November 2015
D. Kane
Ryan Williams
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Abstract

In order to formally understand the power of neural computing, we first need to crack the frontier of threshold circuits with two and three layers, a regime that has been surprisingly intractable to analyze. We prove the first super-linear gate lower bounds and the first super-quadratic wire lower bounds for depth-two linear threshold circuits with arbitrary weights, and depth-three majority circuits computing an explicit function. ∙\bullet∙ We prove that for all ϵ≫log⁡(n)/n\epsilon\gg \sqrt{\log(n)/n}ϵ≫log(n)/n​, the linear-time computable Andreev's function cannot be computed on a (1/2+ϵ)(1/2+\epsilon)(1/2+ϵ)-fraction of nnn-bit inputs by depth-two linear threshold circuits of o(ϵ3n3/2/log⁡3n)o(\epsilon^3 n^{3/2}/\log^3 n)o(ϵ3n3/2/log3n) gates, nor can it be computed with o(ϵ3n5/2/log⁡7/2n)o(\epsilon^{3} n^{5/2}/\log^{7/2} n)o(ϵ3n5/2/log7/2n) wires. This establishes an average-case ``size hierarchy'' for threshold circuits, as Andreev's function is computable by uniform depth-two circuits of o(n3)o(n^3)o(n3) linear threshold gates, and by uniform depth-three circuits of O(n)O(n)O(n) majority gates. ∙\bullet∙ We present a new function in PPP based on small-biased sets, which we prove cannot be computed by a majority vote of depth-two linear threshold circuits with o(n3/2/log⁡3n)o(n^{3/2}/\log^3 n)o(n3/2/log3n) gates, nor with o(n5/2/log⁡7/2n)o(n^{5/2}/\log^{7/2}n)o(n5/2/log7/2n) wires. ∙\bullet∙ We give tight average-case (gate and wire) complexity results for computing PARITY with depth-two threshold circuits; the answer turns out to be the same as for depth-two majority circuits. The key is a new random restriction lemma for linear threshold functions. Our main analytical tool is the Littlewood-Offord Lemma from additive combinatorics.

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