{"created":"2021-03-01T06:05:57.351521+00:00","id":2256,"links":{},"metadata":{"_buckets":{"deposit":"b5cff8b2-ba6f-4911-94a3-3773c3304ba7"},"_deposit":{"id":"2256","owners":[],"pid":{"revision_id":0,"type":"depid","value":"2256"},"status":"published"},"_oai":{"id":"oai:niigata-u.repo.nii.ac.jp:00002256","sets":["176:488:489","453:454"]},"item_5_biblio_info_6":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2010-12","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"Supplement 1","bibliographicPageEnd":"S702","bibliographicPageStart":"S701","bibliographicVolumeNumber":"470","bibliographic_titles":[{"bibliographic_title":"Physica. C, Superconductivity and its applications"},{"bibliographic_title":"Physica. C, Superconductivity and its applications","bibliographic_titleLang":"en"}]}]},"item_5_description_4":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"We investigate the Hubbard–Holstein model by using the dynamical mean-field theory combined with the exact diagonalization method. Below a critical temperature Tcr, a coexistence of two solutions, small lattice fluctuating solution (polaronic state) and large one (bipolaronic state), is found for the same value of the electron–phonon coupling g in the range gc1Tp, while it is single-well type for T