1968
DOI: 10.1016/0375-9601(68)91055-4
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Measurements of κ1(t) and κ2(t) in TaNb alloys

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Cited by 2 publications
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“…It is possible however to develop a theory for κ 2 in superconductors with arbitrary impurity concentration 48,49 . In single-band superconductors κ 2 (T → 0) diverges in the clean limit but for experimentally relevant finite impurity concentrations the changes are not dramatic as compared to the dirty limit 51 . On the other hand in the multiband case an interplay between different Fermi velocities and impurity scattering rates should result in a non-trivial modifications of κ 2 (T ) temperature dependencies.…”
Section: Multiband Superconductors In Large Magnetic Fieldsmentioning
confidence: 95%
See 1 more Smart Citation
“…It is possible however to develop a theory for κ 2 in superconductors with arbitrary impurity concentration 48,49 . In single-band superconductors κ 2 (T → 0) diverges in the clean limit but for experimentally relevant finite impurity concentrations the changes are not dramatic as compared to the dirty limit 51 . On the other hand in the multiband case an interplay between different Fermi velocities and impurity scattering rates should result in a non-trivial modifications of κ 2 (T ) temperature dependencies.…”
Section: Multiband Superconductors In Large Magnetic Fieldsmentioning
confidence: 95%
“…The theoretical calculations were found to be in good agreement with experimentally measured κ 2 (T ) dependencies in several superconducting alloys. [51][52][53] The parameter κ 2 is a basic quantity of type-II superconductors determining their thermodynamic 54 and transport properties 55,56 We consider multiband superconductors in a dirty limit using the Usadel theory 31 . Each k-th band is described in terms of the quasiclassical Green's function matrix ĝk = ĝk (ε, r) which is defined as follows…”
Section: Introductionmentioning
confidence: 99%