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dc.contributor.authorIsakov, Sergei V.en_US
dc.contributor.authorChien, Hong-Chien_US
dc.contributor.authorWu, Jian-Jhengen_US
dc.contributor.authorChen, Yung-Chungen_US
dc.contributor.authorChung, Chung-Houen_US
dc.contributor.authorSengupta, Krishnenduen_US
dc.contributor.authorKim, Yong Baeken_US
dc.date.accessioned2014-12-08T15:08:59Z-
dc.date.available2014-12-08T15:08:59Z-
dc.date.issued2009-08-01en_US
dc.identifier.issn0295-5075en_US
dc.identifier.urihttp://dx.doi.org/10.1209/0295-5075/87/36002en_US
dc.identifier.urihttp://hdl.handle.net/11536/6837-
dc.description.abstractWe investigate the interplay between commensurate lock-in and incommensurate supersolid phases of the hard-core bosons at half-filling with anisotropic nearest-neighbor hopping and repulsive interactions on triangular lattice. We use numerical quantum and variational Monte Carlo as well as analytical Schwinger boson mean-field analysis to establish the ground states and phase diagram. It is shown that, for finite-size systems, there exist a series of jumps between different supersolid phases as the anisotropy parameter is changed. The density ordering wave vectors are locked to commensurate values and jump between adjacent supersolids. In the thermodynamic limit, however, the magnitude of these jumps vanishes leading to a continuous set of novel incommensurate supersolid phases. Copyright (C) EPLA, 2009en_US
dc.language.isoen_USen_US
dc.titleCommensurate lock-in and incommensurate supersolid phases of hard-core bosons on anisotropic triangular latticesen_US
dc.typeArticleen_US
dc.identifier.doi10.1209/0295-5075/87/36002en_US
dc.identifier.journalEPLen_US
dc.citation.volume87en_US
dc.citation.issue3en_US
dc.citation.epageen_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000269610700017-
dc.citation.woscount1-
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