Matches in SemOpenAlex for { <https://semopenalex.org/work/W1998021372> ?p ?o ?g. }
- W1998021372 endingPage "9" @default.
- W1998021372 startingPage "1" @default.
- W1998021372 abstract "The generalized London equation in the mixed state of high-κ s-wave pairing superconductors with impurities is considered as a projection of the quasiclassical nonlocal nonlinear Eilenberger theory. Only one fitting parameter – the cutoff parameter ξh – is used in the theory. The distribution of the magnetic field is calculated self-consistently. Both nonlocal effects originated from extended states between the vortices and bound Andreev states in the vortex are taken into account. Comparison with different analytical nonlocal linear approaches (the Kogan–Gurevich, Amin–Franz–Affleck, Kogan–Zhelezina models) including only extended states is done. The importance of the Kramer–Pesch nonlinear effect and the field dependence of the cutoff parameter is emphasized and their strong influence on the variance of the magnetic field is found. The influence of the impurities on the ratio of the cutoff parameter ξh and the Ginzburg–Landau coherence length ξc2 is considered. Quasiparticle scattering by impurities and lowering of the temperature reduces the value of ξh to the values much less than ξc2. This is different from the prediction of the local Ginzburg–Landau theory where ξh is scaled by ξc2. It is found that impurities influence by different way on the cutoff parameter ξh and the order parameter coherence length ξ1. The ξh decreases monotonously with the impurity scattering time in contrast to the nonmonotonous behavior of ξ1. The results can be used for analysis of the μSR experimental data." @default.
- W1998021372 created "2016-06-24" @default.
- W1998021372 creator A5046717258 @default.
- W1998021372 creator A5050815472 @default.
- W1998021372 creator A5054547958 @default.
- W1998021372 creator A5065844311 @default.
- W1998021372 creator A5087972946 @default.
- W1998021372 date "2012-06-01" @default.
- W1998021372 modified "2023-09-30" @default.
- W1998021372 title "Generalized London theory of the mixed state of high-κ superconductors as a projection of the quasiclassical Eilenberger approach" @default.
- W1998021372 cites W1562553021 @default.
- W1998021372 cites W1603299409 @default.
- W1998021372 cites W1630527847 @default.
- W1998021372 cites W1671339157 @default.
- W1998021372 cites W1828199421 @default.
- W1998021372 cites W1964340667 @default.
- W1998021372 cites W1970755623 @default.
- W1998021372 cites W1973904570 @default.
- W1998021372 cites W1975116420 @default.
- W1998021372 cites W1976979126 @default.
- W1998021372 cites W1978086330 @default.
- W1998021372 cites W1981352426 @default.
- W1998021372 cites W1982416983 @default.
- W1998021372 cites W1986938466 @default.
- W1998021372 cites W1989045471 @default.
- W1998021372 cites W1990533424 @default.
- W1998021372 cites W1993342339 @default.
- W1998021372 cites W1993654550 @default.
- W1998021372 cites W1993719403 @default.
- W1998021372 cites W1994350370 @default.
- W1998021372 cites W1997610401 @default.
- W1998021372 cites W2001031095 @default.
- W1998021372 cites W2001567099 @default.
- W1998021372 cites W2003391620 @default.
- W1998021372 cites W2010920821 @default.
- W1998021372 cites W2012110218 @default.
- W1998021372 cites W2013170175 @default.
- W1998021372 cites W2016848159 @default.
- W1998021372 cites W2017413049 @default.
- W1998021372 cites W2020765206 @default.
- W1998021372 cites W2022084594 @default.
- W1998021372 cites W2025569614 @default.
- W1998021372 cites W2028607546 @default.
- W1998021372 cites W2029110760 @default.
- W1998021372 cites W2029178752 @default.
- W1998021372 cites W2030994956 @default.
- W1998021372 cites W2038985532 @default.
- W1998021372 cites W2042647953 @default.
- W1998021372 cites W2049229411 @default.
- W1998021372 cites W2050378816 @default.
- W1998021372 cites W2055564401 @default.
- W1998021372 cites W2055564641 @default.
- W1998021372 cites W2062958095 @default.
- W1998021372 cites W2068583835 @default.
- W1998021372 cites W2078992519 @default.
- W1998021372 cites W2081167742 @default.
- W1998021372 cites W2086748583 @default.
- W1998021372 cites W2090922956 @default.
- W1998021372 cites W2091022212 @default.
- W1998021372 cites W2091892860 @default.
- W1998021372 cites W2091912007 @default.
- W1998021372 cites W2124310695 @default.
- W1998021372 cites W2131708002 @default.
- W1998021372 cites W2156156126 @default.
- W1998021372 cites W2166647264 @default.
- W1998021372 cites W2237522971 @default.
- W1998021372 cites W3021400620 @default.
- W1998021372 cites W3099372157 @default.
- W1998021372 doi "https://doi.org/10.1016/j.physc.2012.01.019" @default.
- W1998021372 hasPublicationYear "2012" @default.
- W1998021372 type Work @default.
- W1998021372 sameAs 1998021372 @default.
- W1998021372 citedByCount "3" @default.
- W1998021372 countsByYear W19980213722013 @default.
- W1998021372 countsByYear W19980213722014 @default.
- W1998021372 crossrefType "journal-article" @default.
- W1998021372 hasAuthorship W1998021372A5046717258 @default.
- W1998021372 hasAuthorship W1998021372A5050815472 @default.
- W1998021372 hasAuthorship W1998021372A5054547958 @default.
- W1998021372 hasAuthorship W1998021372A5065844311 @default.
- W1998021372 hasAuthorship W1998021372A5087972946 @default.
- W1998021372 hasConcept C115260700 @default.
- W1998021372 hasConcept C121332964 @default.
- W1998021372 hasConcept C124932887 @default.
- W1998021372 hasConcept C136479403 @default.
- W1998021372 hasConcept C140820882 @default.
- W1998021372 hasConcept C158622935 @default.
- W1998021372 hasConcept C163192330 @default.
- W1998021372 hasConcept C168553754 @default.
- W1998021372 hasConcept C174084160 @default.
- W1998021372 hasConcept C191486275 @default.
- W1998021372 hasConcept C26873012 @default.
- W1998021372 hasConcept C2778217198 @default.
- W1998021372 hasConcept C2780360823 @default.
- W1998021372 hasConcept C2781181686 @default.
- W1998021372 hasConcept C54101563 @default.
- W1998021372 hasConcept C62520636 @default.
- W1998021372 hasConcept C71987851 @default.