Matches in SemOpenAlex for { <https://semopenalex.org/work/W2009450167> ?p ?o ?g. }
- W2009450167 endingPage "9513" @default.
- W2009450167 startingPage "9508" @default.
- W2009450167 abstract "A ${d}_{{x}^{2}ensuremath{-}{y}^{2}}$ superconductor is modeled as the superconducting layers in the $aensuremath{-}b$ plane, whose coupling in the c direction is approximated by the effective mass, within the Ginzburg-Landau theory. In this work, this model is applied to the system where the coherence length along the c direction is greater than the layer spacing. Based on our model, we calculate the upper critical field in a magnetic field lying in $aensuremath{-}c$ plane and tilted by an angle from the c axis. According to our results, the curvature of ${H}_{c2}(T)$ is upward, and the slope $ensuremath{-}{mathrm{dH}}_{c2}(T)/dT$ depends on the angle between the c axis and the external field. The most interesting feature is that the ratio of the c-direction parameter related to the effective mass to the $aensuremath{-}b$ plane parameter connected with the effective mass can influence ${H}_{c2}.$ As the ratio is decreased, ${H}_{c2}$ becomes increased. We also find that there is no admixture of s-wave component in the critical regime and believe that the upward curvature of the ${H}_{c2}(T)$ is the characteristic property of a d-wave superconductor." @default.
- W2009450167 created "2016-06-24" @default.
- W2009450167 creator A5019441456 @default.
- W2009450167 creator A5020851000 @default.
- W2009450167 creator A5057244356 @default.
- W2009450167 date "1999-04-01" @default.
- W2009450167 modified "2023-10-16" @default.
- W2009450167 title "Exact solution of the Ginzburg-Landau equation for the upper critical field of adx2−y2superconductor" @default.
- W2009450167 cites W125598520 @default.
- W2009450167 cites W1504459803 @default.
- W2009450167 cites W1563251661 @default.
- W2009450167 cites W1579476841 @default.
- W2009450167 cites W158224491 @default.
- W2009450167 cites W1597228728 @default.
- W2009450167 cites W1610172741 @default.
- W2009450167 cites W1628851465 @default.
- W2009450167 cites W1665657528 @default.
- W2009450167 cites W1667025645 @default.
- W2009450167 cites W1971237570 @default.
- W2009450167 cites W1982376654 @default.
- W2009450167 cites W1987598609 @default.
- W2009450167 cites W1990840069 @default.
- W2009450167 cites W1997308517 @default.
- W2009450167 cites W2001262102 @default.
- W2009450167 cites W2003397470 @default.
- W2009450167 cites W2014850435 @default.
- W2009450167 cites W2034573666 @default.
- W2009450167 cites W2035854066 @default.
- W2009450167 cites W2038844914 @default.
- W2009450167 cites W2041030151 @default.
- W2009450167 cites W2045015840 @default.
- W2009450167 cites W2045296086 @default.
- W2009450167 cites W2052778262 @default.
- W2009450167 cites W2056641878 @default.
- W2009450167 cites W2059987383 @default.
- W2009450167 cites W2061152876 @default.
- W2009450167 cites W2062958095 @default.
- W2009450167 cites W2064042410 @default.
- W2009450167 cites W2064787070 @default.
- W2009450167 cites W2075444143 @default.
- W2009450167 cites W2076621914 @default.
- W2009450167 cites W2078877274 @default.
- W2009450167 cites W2081305238 @default.
- W2009450167 cites W2086748583 @default.
- W2009450167 cites W2094324587 @default.
- W2009450167 cites W2094685470 @default.
- W2009450167 cites W2152769801 @default.
- W2009450167 cites W2168631136 @default.
- W2009450167 cites W23936513 @default.
- W2009450167 cites W2592841103 @default.
- W2009450167 cites W3101347488 @default.
- W2009450167 cites W4367329925 @default.
- W2009450167 cites W613627 @default.
- W2009450167 cites W65296486 @default.
- W2009450167 doi "https://doi.org/10.1103/physrevb.59.9508" @default.
- W2009450167 hasPublicationYear "1999" @default.
- W2009450167 type Work @default.
- W2009450167 sameAs 2009450167 @default.
- W2009450167 citedByCount "3" @default.
- W2009450167 crossrefType "journal-article" @default.
- W2009450167 hasAuthorship W2009450167A5019441456 @default.
- W2009450167 hasAuthorship W2009450167A5020851000 @default.
- W2009450167 hasAuthorship W2009450167A5057244356 @default.
- W2009450167 hasConcept C115260700 @default.
- W2009450167 hasConcept C121332964 @default.
- W2009450167 hasConcept C127413603 @default.
- W2009450167 hasConcept C131584629 @default.
- W2009450167 hasConcept C163192330 @default.
- W2009450167 hasConcept C168553754 @default.
- W2009450167 hasConcept C17825722 @default.
- W2009450167 hasConcept C179764930 @default.
- W2009450167 hasConcept C195065555 @default.
- W2009450167 hasConcept C202444582 @default.
- W2009450167 hasConcept C2524010 @default.
- W2009450167 hasConcept C26873012 @default.
- W2009450167 hasConcept C33923547 @default.
- W2009450167 hasConcept C37914503 @default.
- W2009450167 hasConcept C48496998 @default.
- W2009450167 hasConcept C54101563 @default.
- W2009450167 hasConcept C62520636 @default.
- W2009450167 hasConcept C78519656 @default.
- W2009450167 hasConcept C9652623 @default.
- W2009450167 hasConceptScore W2009450167C115260700 @default.
- W2009450167 hasConceptScore W2009450167C121332964 @default.
- W2009450167 hasConceptScore W2009450167C127413603 @default.
- W2009450167 hasConceptScore W2009450167C131584629 @default.
- W2009450167 hasConceptScore W2009450167C163192330 @default.
- W2009450167 hasConceptScore W2009450167C168553754 @default.
- W2009450167 hasConceptScore W2009450167C17825722 @default.
- W2009450167 hasConceptScore W2009450167C179764930 @default.
- W2009450167 hasConceptScore W2009450167C195065555 @default.
- W2009450167 hasConceptScore W2009450167C202444582 @default.
- W2009450167 hasConceptScore W2009450167C2524010 @default.
- W2009450167 hasConceptScore W2009450167C26873012 @default.
- W2009450167 hasConceptScore W2009450167C33923547 @default.
- W2009450167 hasConceptScore W2009450167C37914503 @default.
- W2009450167 hasConceptScore W2009450167C48496998 @default.
- W2009450167 hasConceptScore W2009450167C54101563 @default.