3,228 research outputs found

    Upper large deviations for the maximal flow in first passage percolation

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    We consider the standard first passage percolation in Zd\mathbb{Z}^{d} for d≄2d\geq 2 and we denote by ϕnd−1,h(n)\phi_{n^{d-1},h(n)} the maximal flow through the cylinder ]0,n]d−1×]0,h(n)]]0,n]^{d-1} \times ]0,h(n)] from its bottom to its top. Kesten proved a law of large numbers for the maximal flow in dimension three: under some assumptions, ϕnd−1,h(n)/nd−1\phi_{n^{d-1},h(n)} / n^{d-1} converges towards a constant Îœ\nu. We look now at the probability that ϕnd−1,h(n)/nd−1\phi_{n^{d-1},h(n)} / n^{d-1} is greater than Îœ+Ï”\nu + \epsilon for some Ï”>0\epsilon >0, and we show under some assumptions that this probability decays exponentially fast with the volume of the cylinder. Moreover, we prove a large deviations principle for the sequence (ϕnd−1,h(n)/nd−1,n∈N)(\phi_{n^{d-1},h(n)} / n^{d-1}, n\in \mathbb{N}).Comment: 27 pages, 4 figures; small changes of notation

    The spread of a rumor or infection in a moving population

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    We consider the following interacting particle system: There is a ``gas'' of particles, each of which performs a continuous-time simple random walk on Zd\mathbb{Z}^d, with jump rate DAD_A. These particles are called AA-particles and move independently of each other. They are regarded as individuals who are ignorant of a rumor or are healthy. We assume that we start the system with NA(x,0−)N_A(x,0-) AA-particles at xx, and that the NA(x,0−),x∈ZdN_A(x,0-),x\in\mathbb{Z}^d, are i.i.d., mean-ÎŒA\mu_A Poisson random variables. In addition, there are BB-particles which perform continuous-time simple random walks with jump rate DBD_B. We start with a finite number of BB-particles in the system at time 0. BB-particles are interpreted as individuals who have heard a certain rumor or who are infected. The BB-particles move independently of each other. The only interaction is that when a BB-particle and an AA-particle coincide, the latter instantaneously turns into a BB-particle. We investigate how fast the rumor, or infection, spreads. Specifically, if B~(t):={x∈Zd:\widetilde{B}(t):=\{x\in\mathbb{Z}^d: a BB-particle visits xx during [0,t]}[0,t]\} and B(t)=B~(t)+[−1/2,1/2]dB(t)=\widetilde{B}(t)+[-1/2,1/2]^d, then we investigate the asymptotic behavior of B(t)B(t). Our principal result states that if DA=DBD_A=D_B (so that the AA- and BB-particles perform the same random walk), then there exist constants 0<Ci<∞0<C_i<\infty such that almost surely C(C2t)⊂B(t)⊂C(C1t)\mathcal{C}(C_2t)\subset B(t)\subset \mathcal{C}(C_1t) for all large tt, where C(r)=[−r,r]d\mathcal{C}(r)=[-r,r]^d. In a further paper we shall use the results presented here to prove a full ``shape theorem,'' saying that t−1B(t)t^{-1}B(t) converges almost surely to a nonrandom set B0B_0, with the origin as an interior point, so that the true growth rate for B(t)B(t) is linear in tt. If DA≠DBD_A\ne D_B, then we can only prove the upper bound B(t)⊂C(C1t)B(t)\subset \mathcal{C}(C_1t) eventually.Comment: Published at http://dx.doi.org/10.1214/009117905000000413 in the Annals of Probability (http://www.imstat.org/aop/) by the Institute of Mathematical Statistics (http://www.imstat.org

    A problem in one-dimensional diffusion-limited aggregation (DLA) and positive recurrence of Markov chains

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    We consider the following problem in one-dimensional diffusion-limited aggregation (DLA). At time tt, we have an "aggregate" consisting of Z∩[0,R(t)]\Bbb{Z}\cap[0,R(t)] [with R(t)R(t) a positive integer]. We also have N(i,t)N(i,t) particles at ii, i>R(t)i>R(t). All these particles perform independent continuous-time symmetric simple random walks until the first time tâ€Č>tt'>t at which some particle tries to jump from R(t)+1R(t)+1 to R(t)R(t). The aggregate is then increased to the integers in [0,R(tâ€Č)]=[0,R(t)+1][0,R(t')]=[0,R(t)+1] [so that R(tâ€Č)=R(t)+1R(t')=R(t)+1] and all particles which were at R(t)+1R(t)+1 at time tâ€Č−t'{-} are removed from the system. The problem is to determine how fast R(t)R(t) grows as a function of tt if we start at time 0 with R(0)=0R(0)=0 and the N(i,0)N(i,0) i.i.d. Poisson variables with mean ÎŒ>0\mu>0. It is shown that if ÎŒ<1\mu<1, then R(t)R(t) is of order t\sqrt{t}, in a sense which is made precise. It is conjectured that R(t)R(t) will grow linearly in tt if ÎŒ\mu is large enough.Comment: Published in at http://dx.doi.org/10.1214/07-AOP379 the Annals of Probability (http://www.imstat.org/aop/) by the Institute of Mathematical Statistics (http://www.imstat.org

    Diffusion Limited Aggregation on a Cylinder

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    We consider the DLA process on a cylinder G x N. It is shown that this process "grows arms", provided that the base graph G has small enough mixing time. Specifically, if the mixing time of G is at most (log|G|)^(2-\eps), the time it takes the cluster to reach the m-th layer of the cylinder is at most of order m |G|/loglog|G|. In particular we get examples of infinite Cayley graphs of degree 5, for which the DLA cluster on these graphs has arbitrarily small density. In addition, we provide an upper bound on the rate at which the "arms" grow. This bound is valid for a large class of base graphs G, including discrete tori of dimension at least 3. It is also shown that for any base graph G, the density of the DLA process on a G-cylinder is related to the rate at which the arms of the cluster grow. This implies, that for any vertex transitive G, the density of DLA on a G-cylinder is bounded by 2/3.Comment: 1 figur

    Analytical study of catalytic reactors for hydrazine decomposition Quarterly progress report, 15 Jul. - 14 Oct. 1966

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    Computer programs used for formulating and solving integral and differential equations in study of catalytic reactors for hydrazine decompositio

    Analytical study of catalytic reactors for hydrazine decomposition Quarterly progress report no. 1, 15 Apr. - 14 Jul. 1966

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    Analytic study of catalytic reactors for hydrazine decompositio

    Further evidence on game theory, simulated interaction, and unaided judgement for forecasting decisions in conflicts.

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    If people in conflicts can more accurately forecast how others will respond, that should help them to make better decisions. Contrary to expert expectations, earlier research found game theorists' forecasts were less accurate than forecasts from simulated interactions using student role players. To assess whether the game theorists had been disadvantaged by the selection of conflicts, I obtained forecasts for three new conflicts (an escalating international confrontation, a takeover battle in the telecommunications industry, and a personal grievance dispute) of types preferred by game theory experts. As before, students were used as role-players, and others provided forecasts using their judgement. When averaged across eight conflicts including five from earlier research, 102 forecasts by 23 game theorists were no more accurate (31% correct predictions) than 357 forecasts by students who used their unaided judgement (32%). Sixty-two percent of 105 simulated-interaction forecasts were accurate, providing an average error reduction of 47% over game-theorist forecasts. Forecasts can sometimes have value without being strictly accurate. Assessing the forecasts using the alternative criterion of usefulness led to the same conclusions about the relative merits of the methods.accuracy, conflict, forecasting, game theory, judgement, methods, role playing, simulated interaction.
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