137 research outputs found

    Hitting Time of Quantum Walks with Perturbation

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    The hitting time is the required minimum time for a Markov chain-based walk (classical or quantum) to reach a target state in the state space. We investigate the effect of the perturbation on the hitting time of a quantum walk. We obtain an upper bound for the perturbed quantum walk hitting time by applying Szegedy's work and the perturbation bounds with Weyl's perturbation theorem on classical matrix. Based on the definition of quantum hitting time given in MNRS algorithm, we further compute the delayed perturbed hitting time (DPHT) and delayed perturbed quantum hitting time (DPQHT). We show that the upper bound for DPQHT is actually greater than the difference between the square root of the upper bound for a perturbed random walk and the square root of the lower bound for a random walk.Comment: 9 page

    Approximation algorithms for the normalizing constant of Gibbs distributions

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    Consider a family of distributions {πβ}\{\pi_{\beta}\} where XπβX\sim\pi_{\beta} means that P(X=x)=exp(βH(x))/Z(β)\mathbb{P}(X=x)=\exp(-\beta H(x))/Z(\beta). Here Z(β)Z(\beta) is the proper normalizing constant, equal to xexp(βH(x))\sum_x\exp(-\beta H(x)). Then {πβ}\{\pi_{\beta}\} is known as a Gibbs distribution, and Z(β)Z(\beta) is the partition function. This work presents a new method for approximating the partition function to a specified level of relative accuracy using only a number of samples, that is, O(ln(Z(β))ln(ln(Z(β))))O(\ln(Z(\beta))\ln(\ln(Z(\beta)))) when Z(0)1Z(0)\geq1. This is a sharp improvement over previous, similar approaches that used a much more complicated algorithm, requiring O(ln(Z(β))ln(ln(Z(β)))5)O(\ln(Z(\beta))\ln(\ln(Z(\beta)))^5) samples.Comment: Published in at http://dx.doi.org/10.1214/14-AAP1015 the Annals of Applied Probability (http://www.imstat.org/aap/) by the Institute of Mathematical Statistics (http://www.imstat.org

    On Sampling from the Gibbs Distribution with Random Maximum A-Posteriori Perturbations

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    In this paper we describe how MAP inference can be used to sample efficiently from Gibbs distributions. Specifically, we provide means for drawing either approximate or unbiased samples from Gibbs' distributions by introducing low dimensional perturbations and solving the corresponding MAP assignments. Our approach also leads to new ways to derive lower bounds on partition functions. We demonstrate empirically that our method excels in the typical "high signal - high coupling" regime. The setting results in ragged energy landscapes that are challenging for alternative approaches to sampling and/or lower bounds

    Estimation in spin glasses: A first step

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    The Sherrington--Kirkpatrick model of spin glasses, the Hopfield model of neural networks and the Ising spin glass are all models of binary data belonging to the one-parameter exponential family with quadratic sufficient statistic. Under bare minimal conditions, we establish the N\sqrt{N}-consistency of the maximum pseudolikelihood estimate of the natural parameter in this family, even at critical temperatures. Since very little is known about the low and critical temperature regimes of these extremely difficult models, the proof requires several new ideas. The author's version of Stein's method is a particularly useful tool. We aim to introduce these techniques into the realm of mathematical statistics through an example and present some open questions.Comment: Published in at http://dx.doi.org/10.1214/009053607000000109 the Annals of Statistics (http://www.imstat.org/aos/) by the Institute of Mathematical Statistics (http://www.imstat.org
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