{"_buckets": {"deposit": "707e0817-11e6-4015-a568-382fc1895bba"}, "_deposit": {"id": "2620", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "2620"}, "status": "published"}, "_oai": {"id": "oai:niigata-u.repo.nii.ac.jp:00002620"}, "item_5_biblio_info_6": {"attribute_name": "\u66f8\u8a8c\u60c5\u5831", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2001-02", "bibliographicIssueDateType": "Issued"}, "bibliographicIssueNumber": "3", "bibliographicPageEnd": "384", "bibliographicPageStart": "375", "bibliographicVolumeNumber": "19", "bibliographic_titles": [{"bibliographic_title": "The European physical journal. B, Condensed matter physics"}, {"bibliographic_title": "The European physical journal. B, Condensed matter physics", "bibliographic_titleLang": "en"}]}]}, "item_5_description_4": {"attribute_name": "\u6284\u9332", "attribute_value_mlt": [{"subitem_description": "The Mott metal-insulator transition in the two-band Hubbard model in infinite dimensions is studied by using the linearized dynamical mean-field theory recently developed by Bulla and Potthoff. The phase boundary of the metal-insulator transition is obtained analytically as a function of the onsite Coulomb interaction at the d-orbital, the charge-transfer energy between the d- and p-orbitals and the hopping integrals between p \u2212 d, d \u2212 d and p \u2212 p orbitals. The result is in good agreement with the numerical results obtained from the exact diagonalization method.", "subitem_description_type": "Abstract"}]}, "item_5_publisher_7": {"attribute_name": "\u51fa\u7248\u8005", "attribute_value_mlt": [{"subitem_publisher": "EDP Sciences"}]}, "item_5_relation_14": {"attribute_name": "DOI", "attribute_value_mlt": [{"subitem_relation_type_id": {"subitem_relation_type_id_text": "info:doi/10.1007/s100510170313", "subitem_relation_type_select": "DOI"}}]}, "item_5_rights_15": {"attribute_name": "\u6a29\u5229", "attribute_value_mlt": [{"subitem_rights": "Copyright (C) 2001 EDP Sciences"}]}, "item_5_select_19": {"attribute_name": "\u8457\u8005\u7248\u30d5\u30e9\u30b0", "attribute_value_mlt": [{"subitem_select_item": "author"}]}, "item_5_source_id_11": {"attribute_name": "\u66f8\u8a8c\u30ec\u30b3\u30fc\u30c9ID", "attribute_value_mlt": [{"subitem_source_identifier": "AA11185661", "subitem_source_identifier_type": "NCID"}]}, "item_5_source_id_9": {"attribute_name": "ISSN", "attribute_value_mlt": [{"subitem_source_identifier": "14346028", "subitem_source_identifier_type": "ISSN"}]}, "item_creator": {"attribute_name": "\u8457\u8005", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "Ono, Y."}], "nameIdentifiers": [{"nameIdentifier": "62", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Bulla, R."}], "nameIdentifiers": [{"nameIdentifier": "38141", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Hewson, A. C."}], "nameIdentifiers": [{"nameIdentifier": "38142", "nameIdentifierScheme": "WEKO"}]}]}, "item_files": {"attribute_name": "\u30d5\u30a1\u30a4\u30eb\u60c5\u5831", "attribute_type": "file", "attribute_value_mlt": [{"accessrole": "open_date", "date": [{"dateType": "Available", "dateValue": "2019-07-29"}], "displaytype": "detail", "download_preview_message": "", "file_order": 0, "filename": "1027.pdf", "filesize": [{"value": "236.6 kB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_free", "mimetype": "application/pdf", "size": 236600.0, "url": {"label": "1027.pdf", "url": "https://niigata-u.repo.nii.ac.jp/record/2620/files/1027.pdf"}, "version_id": "ae6e91e9-bafa-47be-b7a5-2d44fddf6bde"}]}, "item_language": {"attribute_name": "\u8a00\u8a9e", "attribute_value_mlt": [{"subitem_language": "eng"}]}, "item_resource_type": {"attribute_name": "\u8cc7\u6e90\u30bf\u30a4\u30d7", "attribute_value_mlt": [{"resourcetype": "journal article", "resourceuri": "http://purl.org/coar/resource_type/c_6501"}]}, "item_title": "Phase diagram of the Mott Transition in a two-band Hubbard model in infinite dimensions", "item_titles": {"attribute_name": "\u30bf\u30a4\u30c8\u30eb", "attribute_value_mlt": [{"subitem_title": "Phase diagram of the Mott Transition in a two-band Hubbard model in infinite dimensions"}, {"subitem_title": "Phase diagram of the Mott Transition in a two-band Hubbard model in infinite dimensions", "subitem_title_language": "en"}]}, "item_type_id": "5", "owner": "1", "path": ["453/454", "176/488/489"], "permalink_uri": "http://hdl.handle.net/10191/26871", "pubdate": {"attribute_name": "\u516c\u958b\u65e5", "attribute_value": "2014-04-16"}, "publish_date": "2014-04-16", "publish_status": "0", "recid": "2620", "relation": {}, "relation_version_is_last": true, "title": ["Phase diagram of the Mott Transition in a two-band Hubbard model in infinite dimensions"], "weko_shared_id": null}