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Short Point Lists for CNFs and Stronger Constant-Depth Circuit Hardness

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Abstract · v1

We give a short-description decomposition of bounded-width CNFs. For every fixed ε>0\varepsilon>0, every width-bb CNF on mm variables is an exact disjoint union of at most 2εm2^{\varepsilon m} width-bb CNFs, each determined by 2Oε(b)log⁡(m+1)2^{O_\varepsilon(b)}\log(m+1) satisfying assignments. For every fixed d≥3d\ge3, we prove a worst-case size lower bound of 2Ωd((nlog⁡n)1/(d−1))2^{Ω_d((n\log n)^{1/(d-1)})} against depth-at-most-dd unbounded-fan-in AND/OR circuits with input negations for three polynomial-time Boolean families: inverse trace over binary fields, the Goldreich–Tal trilinear function, and OpenAI's polynomial evaluator with its original parameters. All parameter bits count as inputs. For inverse trace, every such circuit of size at most SS, where n≤S≤2cdn1/(d−1)n\le S\le2^{c_dn^{1/(d-1)}}, has uniform sign correlation at most 2−ηdnlog⁡log⁡S/(log⁡S)d−12^{-η_dn\log\log S/(\log S)^{d-1}}. Here cd,ηd>0c_d,η_d>0 depend only on dd. This improves on the classical parity correlation bound. The lower bounds combine the decomposition with restriction arguments; the correlation bound additionally uses common partial decision trees. We also construct exact nonuniform AND/OR circuits for inverse trace of size 2O(n2/3)2^{O(n^{2/3})} at depth eight and 2O(nlog⁡n)2^{O(\sqrt n\log n)} at depth nine. For every fixed integer h≥2h\ge2, the construction gives depth-(4h+1)(4h+1) circuits of size 2Oh(n1/hlog⁡n)2^{O_h(n^{1/h}\log n)}. The upper bounds implement finite-field evaluation and interpolation using circuits that enumerate intermediate states.

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