完整後設資料紀錄
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dc.contributor.authorLin, J. -Y.en_US
dc.contributor.authorHsieh, Y. S.en_US
dc.contributor.authorChareev, D. A.en_US
dc.contributor.authorVasiliev, A. N.en_US
dc.contributor.authorParsons, Y.en_US
dc.contributor.authorYang, H. D.en_US
dc.date.accessioned2019-04-03T06:35:48Z-
dc.date.available2019-04-03T06:35:48Z-
dc.date.issued2011-12-27en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.84.220507en_US
dc.identifier.urihttp://hdl.handle.net/11536/15030-
dc.description.abstractThe comprehensive low-temperature specific-heat C(T) data identify both an isotropic s-wave and extended s-wave order parameters coexisting in a superconducting single-crystal FeSe with T-c = 8.11 K. The isotropic gap Delta(0) = 1.33 meV on the hole Fermi sheets and the extended s-wave gap Delta = Delta(e)(1+ alpha cos2 phi) with Delta(e) = 1.13 meV and alpha = 0.78 on the electron Fermi sheets. The extended s wave is rather anisotropic, but the low-energy quasiparticle excitations demonstrate no sign of the accidental nodes. The coefficient gamma(H) manifesting the quasiparticle contribution to C is a nonlinear function of the applied magnetic field H in the mixed state in accord with the anisotropic multiorder parameters.en_US
dc.language.isoen_USen_US
dc.titleCoexistence of isotropic and extended s-wave order parameters in FeSe as revealed by low-temperature specific heaten_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.84.220507en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume84en_US
dc.citation.issue22en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000298556700002en_US
dc.citation.woscount82en_US
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