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dc.contributor.authorFeng, Xiao-Yongen_US
dc.contributor.authorDai, Jianhuien_US
dc.contributor.authorChung, Chung-Houen_US
dc.contributor.authorSi, Qimiaoen_US
dc.date.accessioned2019-04-03T06:42:57Z-
dc.date.available2019-04-03T06:42:57Z-
dc.date.issued2013-07-03en_US
dc.identifier.issn0031-9007en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevLett.111.016402en_US
dc.identifier.urihttp://hdl.handle.net/11536/22212-
dc.description.abstractWe investigate the competition between the spin-orbit interaction of itinerant electrons and their Kondo coupling with local moments densely distributed on the honeycomb lattice. We find that the model at half-filling displays a quantum phase transition between topological and Kondo insulators at a nonzero Kondo coupling. In the Kondo-screened case, tuning the electron concentration can lead to a new topological insulator phase. The results suggest that the heavy-fermion phase diagram contains a new regime with a competition among topological, Kondo-coherent and magnetic states, and that the regime may be especially relevant to Kondo lattice systems with 5d-conduction electrons. Finally, we discuss the implications of our results in the context of the recent experiments on SmB6 implicating the surface states of a topological insulator, as well as the existing experiments on the phase transitions in SmB6 under pressure and in CeNiSn under chemical pressure.en_US
dc.language.isoen_USen_US
dc.titleCompeting Topological and Kondo Insulator Phases on a Honeycomb Latticeen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevLett.111.016402en_US
dc.identifier.journalPHYSICAL REVIEW LETTERSen_US
dc.citation.volume111en_US
dc.citation.issue1en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000321278300014en_US
dc.citation.woscount21en_US
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