13 research outputs found

    Beta-gamma tail asymptotics

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    We compute the tail asymptotics of the product of a beta random variable and a generalized gamma random variable which are independent and have general parameters. A special case of these asymptotics were proved and used in a recent work of Bubeck, Mossel, and R\'acz in order to determine the tail asymptotics of the maximum degree of the preferential attachment tree. The proof presented here is simpler and highlights why these asymptotics hold.Comment: 6 page

    Optimal control for diffusions on graphs

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    Starting from a unit mass on a vertex of a graph, we investigate the minimum number of "\emph{controlled diffusion}" steps needed to transport a constant mass pp outside of the ball of radius nn. In a step of a controlled diffusion process we may select any vertex with positive mass and topple its mass equally to its neighbors. Our initial motivation comes from the maximum overhang question in one dimension, but the more general case arises from optimal mass transport problems. On Zd\mathbb{Z}^{d} we show that Θ(nd+2)\Theta( n^{d+2} ) steps are necessary and sufficient to transport the mass. We also give sharp bounds on the comb graph and dd-ary trees. Furthermore, we consider graphs where simple random walk has positive speed and entropy and which satisfy Shannon's theorem, and show that the minimum number of controlled diffusion steps is exp(nh/(1+o(1)))\exp{( n \cdot h / \ell ( 1 + o(1) ))}, where hh is the Avez asymptotic entropy and \ell is the speed of random walk. As examples, we give precise results on Galton-Watson trees and the product of trees Td×Tk\mathbb{T}_d \times \mathbb{T}_k.Comment: 32 pages, 2 figure

    Modeling Flocks and Prices: Jumping Particles with an Attractive Interaction

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    We introduce and investigate a new model of a finite number of particles jumping forward on the real line. The jump lengths are independent of everything, but the jump rate of each particle depends on the relative position of the particle compared to the center of mass of the system. The rates are higher for those left behind, and lower for those ahead of the center of mass, providing an attractive interaction keeping the particles together. We prove that in the fluid limit, as the number of particles goes to infinity, the evolution of the system is described by a mean field equation that exhibits traveling wave solutions. A connection to extreme value statistics is also provided.Comment: 35 pages, 9 figures. A shortened version appears as arXiv:1108.243

    A Smooth Transition from Powerlessness to Absolute Power

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    We study the phase transition of the coalitional manipulation problem for generalized scoring rules. Previously it has been shown that, under some conditions on the distribution of votes, if the number of manipulators is o(n)o(\sqrt{n}), where nn is the number of voters, then the probability that a random profile is manipulable by the coalition goes to zero as the number of voters goes to infinity, whereas if the number of manipulators is ω(n)\omega(\sqrt{n}), then the probability that a random profile is manipulable goes to one. Here we consider the critical window, where a coalition has size cnc\sqrt{n}, and we show that as cc goes from zero to infinity, the limiting probability that a random profile is manipulable goes from zero to one in a smooth fashion, i.e., there is a smooth phase transition between the two regimes. This result analytically validates recent empirical results, and suggests that deciding the coalitional manipulation problem may be of limited computational hardness in practice.Comment: 22 pages; v2 contains minor changes and corrections; v3 contains minor changes after comments of reviewer

    A quantitative Gibbard-Satterthwaite theorem without neutrality

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    Recently, quantitative versions of the Gibbard-Satterthwaite theorem were proven for k=3k=3 alternatives by Friedgut, Kalai, Keller and Nisan and for neutral functions on k4k \geq 4 alternatives by Isaksson, Kindler and Mossel. We prove a quantitative version of the Gibbard-Satterthwaite theorem for general social choice functions for any number k3k \geq 3 of alternatives. In particular we show that for a social choice function ff on k3k \geq 3 alternatives and nn voters, which is ϵ\epsilon-far from the family of nonmanipulable functions, a uniformly chosen voter profile is manipulable with probability at least inverse polynomial in nn, kk, and ϵ1\epsilon^{-1}. Removing the neutrality assumption of previous theorems is important for multiple reasons. For one, it is known that there is a conflict between anonymity and neutrality, and since most common voting rules are anonymous, they cannot always be neutral. Second, virtual elections are used in many applications in artificial intelligence, where there are often restrictions on the outcome of the election, and so neutrality is not a natural assumption in these situations. Ours is a unified proof which in particular covers all previous cases established before. The proof crucially uses reverse hypercontractivity in addition to several ideas from the two previous proofs. Much of the work is devoted to understanding functions of a single voter, and in particular we also prove a quantitative Gibbard-Satterthwaite theorem for one voter.Comment: 46 pages; v2 has minor structural changes and adds open problem
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