1995
DOI: 10.1103/physrevb.51.6531
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Effective Lagrangians for BCS superconductors atT=0

Abstract: We show that the low frequency, long wavelength dynamics of the phase of the pair field for a BCS-type s-wave superconductor at T=0 is equivalent to that of a time-dependent non-linear Schrödinger Lagrangian (TDNLSL), when terms required by Galilean invariance are included. If the modulus of the pair field is also allowed to vary, the system is equivalent to two coupled TDNLSL's. 67.50.Fi

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Cited by 101 publications
(179 citation statements)
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“…The system that we have in mind is the dilute Bose gas, which is governed by the Gross-Pitaevskii equation [8,9] at temperatures sufficiently low that the system may be described as a superfluid. It should, however, be noted that this type of equation is applicable to a wider class of systems than just zero-temperature dilute gases [10,11].…”
Section: Introductionmentioning
confidence: 99%
“…The system that we have in mind is the dilute Bose gas, which is governed by the Gross-Pitaevskii equation [8,9] at temperatures sufficiently low that the system may be described as a superfluid. It should, however, be noted that this type of equation is applicable to a wider class of systems than just zero-temperature dilute gases [10,11].…”
Section: Introductionmentioning
confidence: 99%
“…The tadpole to one-loop order is given by (4.7). From the explicit form of the one-loop self-energies in the static limit (5.9), find that 10) which is an exact relationship to one-loop order, obtained for arbitrary ∆ 0 . Upon collecting the above results, we find to one-loop order that…”
Section: Ward Identity and Static Self-energiesmentioning
confidence: 99%
“…While previous efforts, notably by Aitchison et al [10,14], focused on the long-wavelength, low-frequency effective action well below the critical temperature for 0 < T < 0.6 T c our goal is to study the critical region |∆ 0 (T )| ≪ T c with ∆ 0 (T ) the finite-temperature gap. Our study is different from previous attempts in several respects: (i) We implement the Schwinger-Keldysh formulation of nonequilibrium field theory [28] along with the recently introduced tadpole method [31] to obtain the equations of motion for small amplitude fluctuations of the order parameter in real time.…”
Section: Introductionmentioning
confidence: 99%
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“…As it was shown earlier [15,13], in 2D case it is convenient to pass from φ and φ * fields to new variables, namely: the absolute value ρ and the phase θ, where φ(x) = ρ(x) exp[−2iθ(x)], and to perform simultaneously the spinor transformation…”
Section: Model and Main Equationsmentioning
confidence: 99%