31,322 research outputs found

    Algorithms and lower bounds for de Morgan formulas of low-communication leaf gates

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    The class FORMULA[s]∘GFORMULA[s] \circ \mathcal{G} consists of Boolean functions computable by size-ss de Morgan formulas whose leaves are any Boolean functions from a class G\mathcal{G}. We give lower bounds and (SAT, Learning, and PRG) algorithms for FORMULA[n1.99]∘GFORMULA[n^{1.99}]\circ \mathcal{G}, for classes G\mathcal{G} of functions with low communication complexity. Let R(k)(G)R^{(k)}(\mathcal{G}) be the maximum kk-party NOF randomized communication complexity of G\mathcal{G}. We show: (1) The Generalized Inner Product function GIPnkGIP^k_n cannot be computed in FORMULA[s]∘GFORMULA[s]\circ \mathcal{G} on more than 1/2+Ξ΅1/2+\varepsilon fraction of inputs for s=o ⁣(n2(kβ‹…4kβ‹…R(k)(G)β‹…log⁑(n/Ξ΅)β‹…log⁑(1/Ξ΅))2). s = o \! \left ( \frac{n^2}{ \left(k \cdot 4^k \cdot {R}^{(k)}(\mathcal{G}) \cdot \log (n/\varepsilon) \cdot \log(1/\varepsilon) \right)^{2}} \right). As a corollary, we get an average-case lower bound for GIPnkGIP^k_n against FORMULA[n1.99]∘PTFkβˆ’1FORMULA[n^{1.99}]\circ PTF^{k-1}. (2) There is a PRG of seed length n/2+O(sβ‹…R(2)(G)β‹…log⁑(s/Ξ΅)β‹…log⁑(1/Ξ΅))n/2 + O\left(\sqrt{s} \cdot R^{(2)}(\mathcal{G}) \cdot\log(s/\varepsilon) \cdot \log (1/\varepsilon) \right) that Ξ΅\varepsilon-fools FORMULA[s]∘GFORMULA[s] \circ \mathcal{G}. For FORMULA[s]∘LTFFORMULA[s] \circ LTF, we get the better seed length O(n1/2β‹…s1/4β‹…log⁑(n)β‹…log⁑(n/Ξ΅))O\left(n^{1/2}\cdot s^{1/4}\cdot \log(n)\cdot \log(n/\varepsilon)\right). This gives the first non-trivial PRG (with seed length o(n)o(n)) for intersections of nn half-spaces in the regime where Ρ≀1/n\varepsilon \leq 1/n. (3) There is a randomized 2nβˆ’t2^{n-t}-time #\#SAT algorithm for FORMULA[s]∘GFORMULA[s] \circ \mathcal{G}, where t=Ξ©(nsβ‹…log⁑2(s)β‹…R(2)(G))1/2.t=\Omega\left(\frac{n}{\sqrt{s}\cdot\log^2(s)\cdot R^{(2)}(\mathcal{G})}\right)^{1/2}. In particular, this implies a nontrivial #SAT algorithm for FORMULA[n1.99]∘LTFFORMULA[n^{1.99}]\circ LTF. (4) The Minimum Circuit Size Problem is not in FORMULA[n1.99]∘XORFORMULA[n^{1.99}]\circ XOR. On the algorithmic side, we show that FORMULA[n1.99]∘XORFORMULA[n^{1.99}] \circ XOR can be PAC-learned in time 2O(n/log⁑n)2^{O(n/\log n)}

    An average-case depth hierarchy theorem for Boolean circuits

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    We prove an average-case depth hierarchy theorem for Boolean circuits over the standard basis of AND\mathsf{AND}, OR\mathsf{OR}, and NOT\mathsf{NOT} gates. Our hierarchy theorem says that for every dβ‰₯2d \geq 2, there is an explicit nn-variable Boolean function ff, computed by a linear-size depth-dd formula, which is such that any depth-(dβˆ’1)(d-1) circuit that agrees with ff on (1/2+on(1))(1/2 + o_n(1)) fraction of all inputs must have size exp⁑(nΞ©(1/d)).\exp({n^{\Omega(1/d)}}). This answers an open question posed by H{\aa}stad in his Ph.D. thesis. Our average-case depth hierarchy theorem implies that the polynomial hierarchy is infinite relative to a random oracle with probability 1, confirming a conjecture of H{\aa}stad, Cai, and Babai. We also use our result to show that there is no "approximate converse" to the results of Linial, Mansour, Nisan and Boppana on the total influence of small-depth circuits, thus answering a question posed by O'Donnell, Kalai, and Hatami. A key ingredient in our proof is a notion of \emph{random projections} which generalize random restrictions

    Distillation protocols for Fourier states in quantum computing

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    Fourier states are multi-qubit registers that facilitate phase rotations in fault-tolerant quantum computing. We propose distillation protocols for constructing the fundamental, nn-qubit Fourier state with error O(2βˆ’n)O(2^{-n}) at a cost of O(nlog⁑n)O(n \log n) Toffoli gates and Clifford gates, or any arbitrary Fourier state using O(n2)O(n^2) gates. We analyze these protocols with methods from digital signal processing. These results suggest that phase kickback, which uses Fourier states, could be the current lowest-overhead method for generating arbitrary phase rotations.Comment: 18 pages, 4 figure
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