20,019 research outputs found

    Law of large numbers for critical first-passage percolation on the triangular lattice

    Full text link
    We study the site version of (independent) first-passage percolation on the triangular lattice T\mathbb{T}. Denote the passage time of the site vv in T\mathbb{T} by t(v)t(v), and assume that P(t(v)=0)=P(t(v)=1)=1/2P(t(v)=0)=P(t(v)=1)=1/2. Denote by a0,na_{0,n} the passage time from 0\textbf{0} to (n,0)(n,0), and by b0,nb_{0,n} the passage time from 0\textbf{0} to the halfplane {(x,y):xn}\{(x,y):x\geq n\}. We prove that there exists a constant 0<μ<0<\mu<\infty such that as nn\rightarrow\infty, a0,n/lognμa_{0,n}/\log n\rightarrow \mu in probability and b0,n/lognμ/2b_{0,n}/\log n\rightarrow \mu/2 almost surely. This result confirms a prediction of Kesten and Zhang (Probab. Theory Relat. Fields \textbf{107}: 137--160, 1997). The proof relies on the existence of the full scaling limit of critical site percolation on T\mathbb{T}, established by Camia and Newman.Comment: 14 pages, 2 figure

    Limit theorems for critical first-passage percolation on the triangular lattice

    Full text link
    Consider (independent) first-passage percolation on the sites of the triangular lattice T\mathbb{T}. Denote the passage time of the site vv in T\mathbb{T} by t(v)t(v), and assume that P(t(v)=0)=P(t(v)=1)=1/2P(t(v)=0)=P(t(v)=1)=1/2. Denote by b0,nb_{0,n} the passage time from 0 to the halfplane \{v\in\mathbb{T}:\mbox{Re}(v)\geq n\}, and by T(0,nu)T(0,nu) the passage time from 0 to the nearest site to nunu, where u=1|u|=1. We prove that as nn\rightarrow\infty, b0,n/logn1/(23π)b_{0,n}/\log n\rightarrow 1/(2\sqrt{3}\pi) a.s., E[b0,n]/logn1/(23π)E[b_{0,n}]/\log n\rightarrow 1/(2\sqrt{3}\pi) and Var[b0,n]/logn2/(33π)1/(2π2)[b_{0,n}]/\log n\rightarrow 2/(3\sqrt{3}\pi)-1/(2\pi^2); T(0,nu)/logn1/(3π)T(0,nu)/\log n\rightarrow 1/(\sqrt{3}\pi) in probability but not a.s., E[T(0,nu)]/logn1/(3π)E[T(0,nu)]/\log n\rightarrow 1/(\sqrt{3}\pi) and Var[T(0,nu)]/logn4/(33π)1/π2[T(0,nu)]/\log n\rightarrow 4/(3\sqrt{3}\pi)-1/\pi^2. This answers a question of Kesten and Zhang (1997) and improves our previous work (2014). From this result, we derive an explicit form of the central limit theorem for b0,nb_{0,n} and T(0,nu)T(0,nu). A key ingredient for the proof is the moment generating function of the conformal radii for conformal loop ensemble CLE6_6, given by Schramm, Sheffield and Wilson (2009).Comment: 18 pages, 1 figur

    A CLT for winding angles of the arms for critical planar percolation

    Full text link
    Consider critical percolation in two dimensions. Under the condition that there are k disjoint alternating black and white arms crossing the annulus A(l,n), we prove a central limit theorem and variance estimates for the winding angles of the arms (as n\rightarrow \infty, l fixed). This result confirms a prediction of Beffara and Nolin (Ann. Probab. 39: 1286--1304, 2011). Using this theorem, we also get a CLT for the multiple-armed incipient infinite cluster (IIC) measures.Comment: 20 pages, 3 figure

    Asymptotics for 2D critical and near-critical first-passage percolation

    Full text link
    We study Bernoulli first-passage percolation (FPP) on the triangular lattice T\mathbb{T} in which sites have 0 and 1 passage times with probability pp and 1p1-p, respectively. Denote by C\mathcal {C}_{\infty} the infinite cluster with 0-time sites when p>pcp>p_c, where pc=1/2p_c=1/2 is the critical probability. Denote by T(0,C)T(0,\mathcal {C}_{\infty}) the passage time from the origin 0 to C\mathcal {C}_{\infty}. First we obtain explicit limit theorem for T(0,C)T(0,\mathcal {C}_{\infty}) as ppcp\searrow p_c. The proof relies on the limit theorem in the critical case, the critical exponent for correlation length and Kesten's scaling relations. Next, for the usual point-to-point passage time a0,na_{0,n} in the critical case, we construct subsequences of sites with different growth rate along the axis. The main tool involves the large deviation estimates on the nesting of CLE6_6 loops derived by Miller, Watson and Wilson (2016). Finally, we apply the limit theorem for critical Bernoulli FPP to a random graph called cluster graph, obtaining explicit strong law of large numbers for graph distance.Comment: 35 pages, 3 figure

    Multi-arm incipient infinite clusters in 2D: scaling limits and winding numbers

    Full text link
    We study the alternating kk-arm incipient infinite cluster (IIC) of site percolation on the triangular lattice T\mathbb{T}. Using Camia and Newman's result that the scaling limit of critical site percolation on T\mathbb{T} is CLE6_6, we prove the existence of the scaling limit of the kk-arm IIC for k=1,2,4k=1,2,4. Conditioned on the event that there are open and closed arms connecting the origin to DR\partial \mathbb{D}_R, we show that the winding number variance of the arms is (3/2+o(1))logR(3/2+o(1))\log R as RR\rightarrow \infty, which confirms a prediction of Wieland and Wilson (2003). Our proof uses two-sided radial SLE6_6 and coupling argument. Using this result we get an explicit form for the CLT of the winding numbers, and get analogous result for the 2-arm IIC, thus improving our earlier result.Comment: 38 pages, 3 figures. arXiv admin note: text overlap with arXiv:math/0605035 by other author

    Complex Linear Physical-Layer Network Coding

    Full text link
    This paper presents the results of a comprehensive investigation of complex linear physical-layer network (PNC) in two-way relay channels (TWRC). A critical question at relay R is as follows: "Given channel gain ratio η=hA/hB\eta = h_A/h_B, where hAh_A and hBh_B are the complex channel gains from nodes A and B to relay R, respectively, what is the optimal coefficients (α,β)(\alpha,\beta) that minimizes the symbol error rate (SER) of wN=αwA+βwBw_N=\alpha w_A+\beta w_B when we attempt to detect wNw_N in the presence of noise?" Our contributions with respect to this question are as follows: (1) We put forth a general Gaussian-integer formulation for complex linear PNC in which α,β,wA,wB\alpha,\beta,w_A, w_B, and wNw_N are elements of a finite field of Gaussian integers, that is, the field of Z[i]/q\mathbb{Z}[i]/q where qq is a Gaussian prime. Previous vector formulation, in which wAw_A, wBw_B, and wNw_N were represented by 22-dimensional vectors and α\alpha and β\beta were represented by 2×22\times 2 matrices, corresponds to a subcase of our Gaussian-integer formulation where qq is real prime only. Extension to Gaussian prime qq, where qq can be complex, gives us a larger set of signal constellations to achieve different rates at different SNR. (2) We show how to divide the complex plane of η\eta into different Voronoi regions such that the η\eta within each Voronoi region share the same optimal PNC mapping (αopt,βopt)(\alpha_{opt},\beta_{opt}). We uncover the structure of the Voronoi regions that allows us to compute a minimum-distance metric that characterizes the SER of wNw_N under optimal PNC mapping (αopt,βopt)(\alpha_{opt},\beta_{opt}). Overall, the contributions in (1) and (2) yield a toolset for a comprehensive understanding of complex linear PNC in Z[i]/q\mathbb{Z}[i]/q. We believe investigation of linear PNC beyond Z[i]/q\mathbb{Z}[i]/q can follow the same approach.Comment: submitted to IEEE Transactions on Information Theor

    On bifurcation of eigenvalues along convex symplectic paths

    Full text link
    We consider a continuously differentiable curve tγ(t)t\mapsto \gamma(t) in the space of 2n×2n2n\times 2n real symplectic matrices, which is the solution of the following ODE: dγdt(t)=J2nA(t)γ(t),γ(0)Sp(2n,R)\frac{\mathrm{d}\gamma}{\mathrm{d}t}(t)=J_{2n}A(t)\gamma(t), \gamma(0)\in\operatorname{Sp}(2n,\mathbb{R}), where J=J2n=def[0IdnIdn0]J=J_{2n}\overset{\text{def}}{=}\begin{bmatrix}0 & \operatorname{Id}_n\\-\operatorname{Id}_n & 0\end{bmatrix} and A:tA(t)A:t\mapsto A(t) is a continuous in the space of 2n×2n2n\times2n real matrices which are symmetric. Under certain convexity assumption (which includes the particular case that A(t)A(t) is strictly positive definite for all tRt\in\mathbb{R}), we investigate the dynamics of the eigenvalues of γ(t)\gamma(t) when tt varies, which are closely related to the stability of such Hamiltonian dynamical systems. We rigorously prove the qualitative behavior of the branching of eigenvalues and explicitly give the first order asymptotics of the eigenvalues. This generalizes classical Krein-Lyubarskii theorem on the analytic bifurcation of the Floquet multipliers under a linear perturbation of the Hamiltonian. As a corollary, we give a rigorous proof of the following statement of Ekeland: {tR:γ(t) has a Krein indefinite eigenvalue of modulus 1}\{t\in\mathbb{R}:\gamma(t)\text{ has a Krein indefinite eigenvalue of modulus }1\} is a discrete set.Comment: 8 figure

    Dynamics of domain wall in charged AdS dilaton black hole spacetime

    Full text link
    For the n1n-1 dimensional FRW domain wall universe induced by nn dimensional charged dilaton black hole, its movement formula in the bulk can be rewrite as the expansion or collapsing of domain wall. By analysing, we found that in this static AdS space, the cosmologic behaviour of domain wall is particularly single. Even more surprising, it exists an anomaly that the domain wall has a motion area outside of horizon, in which it cannot be explained by our classical theory.Comment: 6 pages, 10figure

    Scalable Bayesian Variable Selection for Structured High-dimensional Data

    Full text link
    Variable selection for structured covariates lying on an underlying known graph is a problem motivated by practical applications, and has been a topic of increasing interest. However, most of the existing methods may not be scalable to high dimensional settings involving tens of thousands of variables lying on known pathways such as the case in genomics studies. We propose an adaptive Bayesian shrinkage approach which incorporates prior network information by smoothing the shrinkage parameters for connected variables in the graph, so that the corresponding coefficients have a similar degree of shrinkage. We fit our model via a computationally efficient expectation maximization algorithm which scalable to high dimensional settings (p~100,000). Theoretical properties for fixed as well as increasing dimensions are established, even when the number of variables increases faster than the sample size. We demonstrate the advantages of our approach in terms of variable selection, prediction, and computational scalability via a simulation study, and apply the method to a cancer genomics study

    A self-organized particle moving model on scale free network with 1/f21/f^{2} behavior

    Full text link
    In this paper we propose a self-organized particle moving model on scale free network with the algorithm of the shortest path and preferential walk. The over-capacity property of the vertices in this particle moving system on complex network is studied from the holistic point of view. Simulation results show that the number of over-capacity vertices forms punctuated equilibrium processes as time elapsing, that the average number of over-capacity vertices under each local punctuated equilibrium process has power law relationship with the local punctuated equilibrium value. What's more, the number of over-capacity vertices has the bell-shaped temporal correlation and 1/f21/f^{2} behavior. Finally, the average lifetime L(t)L(t) of particles accumulated before time tt is analyzed to find the different roles of the shortest path algorithm and the preferential walk algorithm in our model.Comment: 8 pages, 5 figure
    corecore