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dc.contributor.authorDai, MCen_US
dc.contributor.authorYang, TJen_US
dc.contributor.authorTing, CSen_US
dc.date.accessioned2019-04-03T06:39:17Z-
dc.date.available2019-04-03T06:39:17Z-
dc.date.issued1999-04-01en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.59.9508en_US
dc.identifier.urihttp://hdl.handle.net/11536/31408-
dc.description.abstractA d(x2-y2) superconductor is modeled as the superconducting layers in the a-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 a-e 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 - 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 n-b plane parameter connected with the effective mass can influence H-c2. As the rafio 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. [S0163-1829(99)01914-1].en_US
dc.language.isoen_USen_US
dc.titleExact solution of the Ginzburg-Landau equation for the upper critical field of a d(x2-y2) superconductoren_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.59.9508en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume59en_US
dc.citation.issue14en_US
dc.citation.spage9508en_US
dc.citation.epage9513en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000079754300058en_US
dc.citation.woscount3en_US
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