1,123 research outputs found

    An elementary proof for the dimension of the graph of the classical Weierstrass function

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    Let Wλ,b(x)=n=0λng(bnx)W_{\lambda,b}(x)=\sum_{n=0}^\infty\lambda^n g(b^n x) where b2b\geqslant2 is an integer and g(u)=cos(2πu)g(u)=\cos(2\pi u) (classical Weierstrass function). Building on work by Ledrappier (1992), Bar\'ansky, B\'ar\'any and Romanowska (2013) and Tsujii (2001), we provide an elementary proof that the Hausdorff dimension of Wλ,bW_{\lambda,b} equals 2+logλlogb2+\frac{\log\lambda}{\log b} for all λ(λb,1)\lambda\in(\lambda_b,1) with a suitable λb<1\lambda_b<1. This reproduces results by Bar\'ansky, B\'ar\'any and Romanowska without using the dimension theory for hyperbolic measures of Ledrappier and Young (1985,1988), which is replaced by a simple telescoping argument together with a recursive multi-scale estimate.Comment: The proof of Proposition 3.3 is clarified and a mistake is correcte

    Map Lattices coupled by collisions

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    We introduce a new coupled map lattice model in which the weak interaction takes place via rare "collisions". By "collision" we mean a strong (possibly discontinuous) change in the system. For such models we prove uniqueness of the SRB measure and exponential space-time decay of correlations

    Phase transitions in a piecewise expanding coupled map lattice with linear nearest neighbour coupling

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    We construct a mixing continuous piecewise linear map on [-1,1] with the property that a two-dimensional lattice made of these maps with a linear north and east nearest neighbour coupling admits a phase transition. We also provide a modification of this construction where the local map is an expanding analytic circle map. The basic strategy is borroughed from [Gielis-MacKay (2000)], namely we compare the dynamics of the CML to those of a probabilistic cellular automaton of Toom's type.Comment: 19 page

    Random walk in Markovian environment

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    We prove a quenched central limit theorem for random walks with bounded increments in a randomly evolving environment on Zd\mathbb{Z}^d. We assume that the transition probabilities of the walk depend not too strongly on the environment and that the evolution of the environment is Markovian with strong spatial and temporal mixing properties.Comment: Published in at http://dx.doi.org/10.1214/07-AOP369 the Annals of Probability (http://www.imstat.org/aop/) by the Institute of Mathematical Statistics (http://www.imstat.org
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