1981
DOI: 10.1007/bf00117427
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Nonequilibrium theory of dirty, current-carrying superconductors: phase-slip oscillators in narrow filaments near T c

Abstract: General equations for the dynamic behavior of dirty superconductors in theGinzburg-Landau regime ITc-TI << T~ are derived from microscopic theory.In the immediate vicinity of Tc a local equilibrium approximation leads to a simple generalized time-dependent Ginzburg-Landau equation. The oscillatory phase-slip solutions presented previously are discussed in greater detail.

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Cited by 219 publications
(158 citation statements)
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“…In order to explore the dynamic properties in such a superconducting ring, the generalized TDGL equation can be written in the following form; 41,42 where the parameter γ=2τ E ψ 0 / characterizes the material with τ E being the inelastic collision time and ψ 0 being the value of order parameter in the absence of external field at zero temperature. This equation should be coupled with the equation for the electrostatic potential:…”
Section: Theoretical Approachmentioning
confidence: 99%
“…In order to explore the dynamic properties in such a superconducting ring, the generalized TDGL equation can be written in the following form; 41,42 where the parameter γ=2τ E ψ 0 / characterizes the material with τ E being the inelastic collision time and ψ 0 being the value of order parameter in the absence of external field at zero temperature. This equation should be coupled with the equation for the electrostatic potential:…”
Section: Theoretical Approachmentioning
confidence: 99%
“…(4) is limited by gapless superconductivity. In this section, we consider a more general approach based on the generalized TDGL equations 19 (see also Ref. 12 for review):…”
Section: Temperature Dependence Of the Viscosity Anisotropymentioning
confidence: 99%
“…12,19 Note that for Fe-based materials, the gapless regime may be achievable due to the strong interband scattering on dopant's ions. 20 In Sec.…”
Section: Introductionmentioning
confidence: 99%
“…We note that the Lagrangian L[ψ † , ψ, χ † , χ] is obviously invariant under the gauge transformations 16) which, as will be seen below, is at the heart of the Ward identity. Whereas in general a gauge transformation is invoked to fix the condensate ∆ 0 to be real for convenience, this choice corresponds to fixing a particular gauge, which in turn hides the underlying gauge symmetry.…”
Section: B Real-time Relaxation In Linear Responsementioning
confidence: 99%
“…Kopnin [15] studied the nonequilibrium dynamics of flux flow in clean superconductors but did not address the validity of the time dependent Landau-Ginzburg description near the critical point. Watts-Tobin et al [16] studied the validity of the Landau-Ginzburg description near the critical point for dirty superconductors where relaxational processes are dominated by (elastic) collisions.…”
Section: Introductionmentioning
confidence: 99%