mlsanityData to 14 Oct 2026

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

arXiv 1511.07860 ↗First posted 24 Nov 2015cs.CC cs.NEcited by 6

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Abstract (arXiv)

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 εgg √log(n)/n, the linear-time computable Andreev's function cannot be computed on a (1/2+ε)-fraction of n-bit inputs by depth-two linear threshold circuits of o(ε3 n3/2/log3 n) gates, nor can it be computed with o(ε3 n5/2/log7/2 n) 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) linear threshold gates, and by uniform depth-three circuits of O(n) majority gates. bullet We present a new function in P 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/log3 n) gates, nor with 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.

Key facts. Cited by 6 papers in the map (data through 14 Oct 2026). First posted on arXiv 24 Nov 2015.

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Citing papers per year: 2021: 3; 2022: 0; 2023: 1; 2024: 0; 2025: 1; 2026: 1.

6 papers.