528 research outputs found

    Superpolynomial lower bounds for general homogeneous depth 4 arithmetic circuits

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    In this paper, we prove superpolynomial lower bounds for the class of homogeneous depth 4 arithmetic circuits. We give an explicit polynomial in VNP of degree nn in n2n^2 variables such that any homogeneous depth 4 arithmetic circuit computing it must have size nΩ(loglogn)n^{\Omega(\log \log n)}. Our results extend the works of Nisan-Wigderson [NW95] (which showed superpolynomial lower bounds for homogeneous depth 3 circuits), Gupta-Kamath-Kayal-Saptharishi and Kayal-Saha-Saptharishi [GKKS13, KSS13] (which showed superpolynomial lower bounds for homogeneous depth 4 circuits with bounded bottom fan-in), Kumar-Saraf [KS13a] (which showed superpolynomial lower bounds for homogeneous depth 4 circuits with bounded top fan-in) and Raz-Yehudayoff and Fournier-Limaye-Malod-Srinivasan [RY08, FLMS13] (which showed superpolynomial lower bounds for multilinear depth 4 circuits). Several of these results in fact showed exponential lower bounds. The main ingredient in our proof is a new complexity measure of {\it bounded support} shifted partial derivatives. This measure allows us to prove exponential lower bounds for homogeneous depth 4 circuits where all the monomials computed at the bottom layer have {\it bounded support} (but possibly unbounded degree/fan-in), strengthening the results of Gupta et al and Kayal et al [GKKS13, KSS13]. This new lower bound combined with a careful "random restriction" procedure (that transforms general depth 4 homogeneous circuits to depth 4 circuits with bounded support) gives us our final result

    Eroding dipoles and vorticity growth for Euler flows in R 3 : Axisymmetric flow without swirl

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    A review of analyses based upon anti-parallel vortex structures suggests that structurally stable dipoles with eroding circulation may offer a path to the study of vorticity growth in solutions of Euler’s equations in R3 . We examine here the possible formation of such a structure in axisymmetric flow without swirl, leading to maximal growth of vorticity as t 4/3 . Our study suggests that the optimizing flow giving the t 4/3 growth mimics an exact solution of Euler’s equations representing an eroding toroidal vortex dipole which locally conserves kinetic energy. The dipole cross-section is a perturbation of the classical Sadovskii dipole having piecewise constant vorticity, which breaks the symmetry of closed streamlines. The structure of this perturbed Sadovskii dipole is analyzed asymptotically at large times, and its predicted properties are verified numerically. We also show numerically that if mirror symmetry of the dipole is not imposed but axial symmetry maintained, an instability leads to breakup into smaller vortical structures

    Bandit Online Optimization Over the Permutahedron

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    The permutahedron is the convex polytope with vertex set consisting of the vectors (π(1),,π(n))(\pi(1),\dots, \pi(n)) for all permutations (bijections) π\pi over {1,,n}\{1,\dots, n\}. We study a bandit game in which, at each step tt, an adversary chooses a hidden weight weight vector sts_t, a player chooses a vertex πt\pi_t of the permutahedron and suffers an observed loss of i=1nπ(i)st(i)\sum_{i=1}^n \pi(i) s_t(i). A previous algorithm CombBand of Cesa-Bianchi et al (2009) guarantees a regret of O(nTlogn)O(n\sqrt{T \log n}) for a time horizon of TT. Unfortunately, CombBand requires at each step an nn-by-nn matrix permanent approximation to within improved accuracy as TT grows, resulting in a total running time that is super linear in TT, making it impractical for large time horizons. We provide an algorithm of regret O(n3/2T)O(n^{3/2}\sqrt{T}) with total time complexity O(n3T)O(n^3T). The ideas are a combination of CombBand and a recent algorithm by Ailon (2013) for online optimization over the permutahedron in the full information setting. The technical core is a bound on the variance of the Plackett-Luce noisy sorting process's "pseudo loss". The bound is obtained by establishing positive semi-definiteness of a family of 3-by-3 matrices generated from rational functions of exponentials of 3 parameters

    Stochastic Streams: Sample Complexity vs. Space Complexity

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    We address the trade-off between the computational resources needed to process a large data set and the number of samples available from the data set. Specifically, we consider the following abstraction: we receive a potentially infinite stream of IID samples from some unknown distribution D, and are tasked with computing some function f(D). If the stream is observed for time t, how much memory, s, is required to estimate f(D)? We refer to t as the sample complexity and s as the space complexity. The main focus of this paper is investigating the trade-offs between the space and sample complexity. We study these trade-offs for several canonical problems studied in the data stream model: estimating the collision probability, i.e., the second moment of a distribution, deciding if a graph is connected, and approximating the dimension of an unknown subspace. Our results are based on techniques for simulating different classical sampling procedures in this model, emulating random walks given a sequence of IID samples, as well as leveraging a characterization between communication bounded protocols and statistical query algorithms

    Efficient solvability of Hamiltonians and limits on the power of some quantum computational models

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    We consider quantum computational models defined via a Lie-algebraic theory. In these models, specified initial states are acted on by Lie-algebraic quantum gates and the expectation values of Lie algebra elements are measured at the end. We show that these models can be efficiently simulated on a classical computer in time polynomial in the dimension of the algebra, regardless of the dimension of the Hilbert space where the algebra acts. Similar results hold for the computation of the expectation value of operators implemented by a gate-sequence. We introduce a Lie-algebraic notion of generalized mean-field Hamiltonians and show that they are efficiently ("exactly") solvable by means of a Jacobi-like diagonalization method. Our results generalize earlier ones on fermionic linear optics computation and provide insight into the source of the power of the conventional model of quantum computation.Comment: 6 pages; no figure

    Static Data Structure Lower Bounds Imply Rigidity

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    We show that static data structure lower bounds in the group (linear) model imply semi-explicit lower bounds on matrix rigidity. In particular, we prove that an explicit lower bound of tω(log2n)t \geq \omega(\log^2 n) on the cell-probe complexity of linear data structures in the group model, even against arbitrarily small linear space (s=(1+ε)n)(s= (1+\varepsilon)n), would already imply a semi-explicit (PNP\bf P^{NP}\rm) construction of rigid matrices with significantly better parameters than the current state of art (Alon, Panigrahy and Yekhanin, 2009). Our results further assert that polynomial (tnδt\geq n^{\delta}) data structure lower bounds against near-optimal space, would imply super-linear circuit lower bounds for log-depth linear circuits (a four-decade open question). In the succinct space regime (s=n+o(n))(s=n+o(n)), we show that any improvement on current cell-probe lower bounds in the linear model would also imply new rigidity bounds. Our results rely on a new connection between the "inner" and "outer" dimensions of a matrix (Paturi and Pudlak, 2006), and on a new reduction from worst-case to average-case rigidity, which is of independent interest

    Improved bounds for reduction to depth 4 and depth 3

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    Koiran showed that if a nn-variate polynomial of degree dd (with d=nO(1)d=n^{O(1)}) is computed by a circuit of size ss, then it is also computed by a homogeneous circuit of depth four and of size 2O(dlog(d)log(s))2^{O(\sqrt{d}\log(d)\log(s))}. Using this result, Gupta, Kamath, Kayal and Saptharishi gave a exp(O(dlog(d)log(n)log(s)))\exp(O(\sqrt{d\log(d)\log(n)\log(s)})) upper bound for the size of the smallest depth three circuit computing a nn-variate polynomial of degree d=nO(1)d=n^{O(1)} given by a circuit of size ss. We improve here Koiran's bound. Indeed, we show that if we reduce an arithmetic circuit to depth four, then the size becomes exp(O(dlog(ds)log(n)))\exp(O(\sqrt{d\log(ds)\log(n)})). Mimicking Gupta, Kamath, Kayal and Saptharishi's proof, it also implies the same upper bound for depth three circuits. This new bound is not far from optimal in the sense that Gupta, Kamath, Kayal and Saptharishi also showed a 2Ω(d)2^{\Omega(\sqrt{d})} lower bound for the size of homogeneous depth four circuits such that gates at the bottom have fan-in at most d\sqrt{d}. Finally, we show that this last lower bound also holds if the fan-in is at least d\sqrt{d}

    Classical simulation of noninteracting-fermion quantum circuits

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    We show that a class of quantum computations that was recently shown to be efficiently simulatable on a classical computer by Valiant corresponds to a physical model of noninteracting fermions in one dimension. We give an alternative proof of his result using the language of fermions and extend the result to noninteracting fermions with arbitrary pairwise interactions, where gates can be conditioned on outcomes of complete von Neumann measurements in the computational basis on other fermionic modes in the circuit. This last result is in remarkable contrast with the case of noninteracting bosons where universal quantum computation can be achieved by allowing gates to be conditioned on classical bits (quant-ph/0006088).Comment: 26 pages, 1 figure, uses wick.sty; references added to recent results by E. Knil
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