Universality of Flux Creep in Superconductors with Arbitrary Shape and Current-Voltage Law
Ernst Helmut Brandt
DOI 10.1103/PhysRevLett.76.4030 · Physical Review Letters
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Abstract
The nonlinear and nonlocal diffusion equation for the relaxing current density J(r,t) in long superconductors of arbitrary cross section in a constant perpendicular magnetic field Ba is solved exactly by separation of variables in the electric field E(r,t)=f(r)g(t). This solution includes the limiting cases of longitudinal and transverse geometries and applies to the current-voltage laws E∝Jn ranging from Ohmic ( n=1) to Bean-like ( n→∞) behavior. The electric field profile f(r) weakly depends on n and becomes universal for n exceeding ≈5. At large times t one finds E∝1/tn/(n−1) and J∝1/t1/(n−1) for n>1, and E∝J∝exp(−t/τ0) for n=1. The contour lines of the creeping E(r,t) coincide with the field lines of B(r,t) in the remanent state Ba=0.
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