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    Explicit predictability and dispersion scaling exponents in fully developed turbulence

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    We apply a simple method to provide explicit expressions for different scaling exponents in intermittent fully developed turbulence, that before were only given through a Legendre transform. This includes predictability exponents for infinitesimal and non infinitesimal perturbations, Lagrangian velocity exponents, and dispersion exponents. We obtain also new results concerning inverse statistics corresponding to exit-time moments.Comment: Physics Letters A (in press

    Values of Brownian intersection exponents III: Two-sided exponents

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    This paper determines values of intersection exponents between packs of planar Brownian motions in the half-plane and in the plane that were not derived in our first two papers. For instance, it is proven that the exponent ξ(3,3)\xi (3,3) describing the asymptotic decay of the probability of non-intersection between two packs of three independent planar Brownian motions each is (73−273)/12(73-2 \sqrt {73}) / 12. More generally, the values of ξ(w1,>...,wk)\xi (w_1, >..., w_k) and \tx (w_1', ..., w_k') are determined for all k≥2 k \ge 2, w1,w2≥1w_1, w_2\ge 1, w3,...,wk∈[0,∞)w_3, ...,w_k\in[0,\infty) and all w1′,...,wk′∈[0,∞)w_1',...,w_k'\in[0,\infty). The proof relies on the results derived in our first two papers and applies the same general methods. We first find the two-sided exponents for the stochastic Loewner evolution processes in a half-plane, from which the Brownian intersection exponents are determined via a universality argument

    Critical exponents in zero dimensions

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    In the vicinity of the onset of an instability, we investigate the effect of colored multiplicative noise on the scaling of the moments of the unstable mode amplitude. We introduce a family of zero dimensional models for which we can calculate the exact value of the critical exponents βm\beta_m for all the moments. The results are obtained through asymptotic expansions that use the distance to onset as a small parameter. The examined family displays a variety of behaviors of the critical exponents that includes anomalous exponents: exponents that differ from the deterministic (mean-field) prediction, and multiscaling: non-linear dependence of the exponents on the order of the moment
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