{ "id": "cond-mat/0104232", "version": "v1", "published": "2001-04-12T14:55:54.000Z", "updated": "2001-04-12T14:55:54.000Z", "title": "Marginal pinning of vortices at high temperature", "authors": [ "M. Mueller", "D. A. Gorokhov", "G. Blatter" ], "comment": "5 pages, RevTeX, 1 postscript figure inserted", "journal": "Phys. Rev. B 64, 134523 (2001)", "doi": "10.1103/PhysRevB.64.134523", "categories": [ "cond-mat.dis-nn", "cond-mat.stat-mech", "cond-mat.supr-con" ], "abstract": "We analyze the competition between thermal fluctuations and pinning of vortices in bulk type II superconductors subject to point-like disorder and derive an expression for the temperature dependence of the pinning length L_c(T) which separates different types of single vortex wandering. Given a disorder potential with a basic scale \\xi and a correlator K_0(u) \\sim K_0 (u/xi)^{-\\beta} ln^alpha (u/xi) we determine the dependence of L_c(T) on the correlator range: correlators with \\beta > 2 (short-range) and \\beta <2 (long-range) lead to the known results L_c(T) \\sim L_c(0) exp[C T^3] and L_c(T) \\sim L_c(0) (C T)^{(4+beta)/(2-beta)}, respectively. Using functional renormalization group we show that for \\beta =2 the result takes the interpolating form L_c(T) \\sim L_c(0) exp[C T^{3/(2+alpha)}]. Pinning of vortices in bulk type II superconductors involves a long-range correlator with \\beta=2, \\alpha=1 on intermediate scales \\xi