15,370 research outputs found

    Instanton for the Kraichnan Passive Scalar Problem

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    We consider high-order correlation functions of the passive scalar in the Kraichnan model. Using the instanton formalism we find the scaling exponents ζn\zeta_n of the structure functions SnS_n for n1n\gg1 under the additional condition dζ21d\zeta_2\gg1 (where dd is the dimensionality of space). At n<ncn<n_c (where nc=dζ2/[2(2ζ2)]n_c = d\zeta_2/[2(2-\zeta_2)]) the exponents are ζn=(ζ2/4)(2nn2/nc)\zeta_n=(\zeta_2/4)(2n-n^2/n_c), while at n>ncn>n_c they are nn-independent: ζn=ζ2nc/4\zeta_n=\zeta_2 n_c/4. We also estimate nn-dependent factors in SnS_n, particularly their behavior at nn close to ncn_c.Comment: 20 pages, RevTe

    Theory of the Spatio-Temporal Dynamics of Transport Bifurcations

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    The development and time evolution of a transport barrier in a magnetically confined plasma with non-monotonic, nonlinear dependence of the anomalous flux on mean gradients is analyzed. Upon consideration of both the spatial inhomogeneity and the gradient nonlinearity of the transport coefficient, we find that the transition develops as a bifurcation front with radially propagating discontinuity in local gradient. The spatial location of the transport barrier as a function of input flux is calculated. The analysis indicates that for powers slightly above threshold, the barrier location xb(t)(Dnt(PPc)/Pc)1/2,x_b(t) \sim ( D_n t (P-P_c)/P_c)^{1/2}, where PcP_c is the local transition power threshold and DnD_n is the neoclassical diffusivity . This result suggests a simple explanation of the high disruptivity observed in reversed shear plasmas. The basic conclusions of this theory are insensitive to the details of the local transport model.Comment: 21 page Tex file, 10 postscript file
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