1989
DOI: 10.1103/physrevb.39.11307
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Theory of superconducting-quasiparticle interface states

Abstract: We calculate the thermodynamic Green's functions for a BCS superconductor with a wall of magnetic material cleaving it into two semi-infinite regions. This is a model of an interface between a superconductor and a perfectly insulating ferromagnet. We show that the scattering of superconducting quasiparticles from a spin-polarized wall leads to resonant pair breaking and the formation of subgap bands in the tunneling density of states. These bands bear a superficial resemblance to the bands observed in bulk sup… Show more

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Cited by 19 publications
(12 citation statements)
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“…The dimensionless parameter characterizing barrier strength 36 is Z 0 ≡ mH/hk F , where the effective mass, m, is taken to be equal in the F and S regions. In the superconducting region, at x > 0, we assume 6,7,28,36,40 that there is a pair potential…”
Section: Methodsmentioning
confidence: 99%
“…The dimensionless parameter characterizing barrier strength 36 is Z 0 ≡ mH/hk F , where the effective mass, m, is taken to be equal in the F and S regions. In the superconducting region, at x > 0, we assume 6,7,28,36,40 that there is a pair potential…”
Section: Methodsmentioning
confidence: 99%
“…In principle, the pair potential should be determined self-consistently. However, this would greatly complicate the calculations without shedding much light on the exchange-interaction-induced states in the S/F/S case [10,21], which is the main subject of this paper. In the S/N/S case, the validity of our model requires a weak proximity effect in S, as it may be the case at low T and for thin and short barriers.…”
Section: Quasiparticles Green's Functionmentioning
confidence: 99%
“…( 16), one can easily see that ZES can occur for φ = φ gs only. Due to the spin splitting, SPGS may appear [10,11,21]. Analyzing Eq.…”
Section: Densities Of Statesmentioning
confidence: 99%
“…We now show that the decrease in Tc at Hc is related to an interface MEF, which acts on the superconductivity in PCCO within a distance of ξc(T) of the PCCO/PCMO interface. For H > Hc, the PCMO is magnetically saturated, and so the Cooper pairs in PCCO experience a spatially uniform MEF through an exchange interaction [86][87][88][89] with the electrons in Mn 3d eg 1 band at the interface of PCMO, which introduces a spin splitting in the superconducting DOS and an interface suppression of Tc (see related works in [47,48,50,54,55]). However, around Hc, the magnetization in PCMO is inhomogeneous with magnetic domains pointing in different directions with the domain wall density therefore maximized.…”
mentioning
confidence: 99%