2017
DOI: 10.7566/jpsj.86.073702
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Charging due to Pair-Potential Gradient in Vortex of Type-II Superconductors

Abstract: Besides the magnetic Lorentz force familiar from the Hall effect in metals and semiconductors, there exists a mechanism for charging peculiar to superconductors that is caused by the pair-potential gradient (PPG). We incorporate it in the augmented quasiclassical equations of superconductivity with the Lorentz force to study charging of an isolated vortex in an equilibrium s-wave type-II superconductor. It is found that the PPG mechanism gives rise to charging concentrated within the core whose magnitude at th… Show more

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Cited by 8 publications
(29 citation statements)
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“…In the s-wave case, the temperature dependence of the charge density at the origin is studied in Ref. 25. In a similar way, we study the dependence of chiral p-wave cases.…”
Section: B Temperature Dependencementioning
confidence: 96%
See 1 more Smart Citation
“…In the s-wave case, the temperature dependence of the charge density at the origin is studied in Ref. 25. In a similar way, we study the dependence of chiral p-wave cases.…”
Section: B Temperature Dependencementioning
confidence: 96%
“…The phase transformation of the Green's function in real space is convenient to take account of the gauge invariance in the mixed representation. First of all we formulate the augmented quasiclassical theory following the earlier works in the Matsubara formalism 25,26,38 . The Green's function in the mixed representation is introduced as the Fourier transform with respect to the relative coordinate r = r 1 − r 2 of the phase transformed Green's function…”
Section: Formulationmentioning
confidence: 99%
“…We consider type-II superconductors with pinned vortices and neglect the pair-potential-gradient force [51][52][53] and the pressure difference arising from the slope in the density of states (DOS) [54], which only contribute to the vortex-core charging in this case, since the charge in a pinned vortex does not contribute to thermal conductivity. For simplicity, we also restrict ourselves to the spin-singlet pairing without spin paramagnetism.…”
Section: Augmented Quasiclassical Equationsmentioning
confidence: 99%
“…Let us carry out a perturbation expansion with respect to the Lorentz and PPG forces as g R = g R 0 + g R 1 · · · and g R(1) = 29,36,42) which is performed up to the first order in the quasiclassical parameter δ below. We also use Eq.…”
Section: Charge and Current Densitiesmentioning
confidence: 99%