{"_buckets": {"deposit": "26976760-0191-4109-9a4b-1c99cb12de2b"}, "_deposit": {"id": "2263", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "2263"}, "status": "published"}, "_oai": {"id": "oai:niigata-u.repo.nii.ac.jp:00002263"}, "item_5_biblio_info_6": {"attribute_name": "\u66f8\u8a8c\u60c5\u5831", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2004", "bibliographicIssueDateType": "Issued"}, "bibliographicIssueNumber": "15", "bibliographicPageEnd": "155102-7", "bibliographicPageStart": "155102-1", "bibliographicVolumeNumber": "70", "bibliographic_titles": [{"bibliographic_title": "Physical Review B"}, {"bibliographic_title": "Physical Review B", "bibliographic_titleLang": "en"}]}]}, "item_5_description_4": {"attribute_name": "\u6284\u9332", "attribute_value_mlt": [{"subitem_description": "We examine the critical behavior near the metal-insulator transition (MIT) in the one-dimensional extended Hubbard model with the on-site and the nearest-neighbor interactions U and V at quarter filling using a combined method of the numerical diagonalization and the renormalization group (RG). The Luttinger-liquid parameter K\u03c1 is calculated with the exact diagonalization for finite size systems and is substituted into the RG equation as an initial condition to obtain K\u03c1 in the infinite size system. This approach also yields the charge gap \u0394 in the insulating state near the MIT. The results agree very well with the available exact results for U=\u221e even in the critical regime of the MIT where the characteristic energy becomes exponentially small and the usual finite size scaling is not applicable. When the system approaches the MIT critical point V\u2192Vc for a fixed U, K\u03c1 and \u0394 behave as [numerical formula] and [numerical formula], where the critical value Vc and the coefficients c\u0394 and cK are functions of U. These critical properties, which are known to be exact for U=\u221e, are observed also for finite U case. We also observe the same critical behavior in the limit of the MIT critical point U\u2192Uc when U is varied for a fixed V.", "subitem_description_type": "Abstract"}]}, "item_5_full_name_3": {"attribute_name": "\u8457\u8005\u5225\u540d", "attribute_value_mlt": [{"nameIdentifiers": [{"nameIdentifier": "62", "nameIdentifierScheme": "WEKO"}], "names": [{"name": "\u5927\u91ce, \u7fa9\u7ae0"}]}]}, "item_5_publisher_7": {"attribute_name": "\u51fa\u7248\u8005", "attribute_value_mlt": [{"subitem_publisher": "American Physical Society"}]}, "item_5_relation_14": {"attribute_name": "DOI", "attribute_value_mlt": [{"subitem_relation_type_id": {"subitem_relation_type_id_text": "info:doi/10.1103/PhysRevB.70.155102", "subitem_relation_type_select": "DOI"}}]}, "item_5_rights_15": {"attribute_name": "\u6a29\u5229", "attribute_value_mlt": [{"subitem_rights": "The American Physical Society"}]}, "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": "AA11187113", "subitem_source_identifier_type": "NCID"}]}, "item_5_source_id_9": {"attribute_name": "ISSN", "attribute_value_mlt": [{"subitem_source_identifier": "10980121", "subitem_source_identifier_type": "ISSN"}]}, "item_creator": {"attribute_name": "\u8457\u8005", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "Sano, Kazuhiro"}], "nameIdentifiers": [{"nameIdentifier": "7684", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Ono, Yoshiaki"}], "nameIdentifiers": [{"nameIdentifier": "62", "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": "19_0006.pdf", "filesize": [{"value": "276.4 kB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_free", "mimetype": "application/pdf", "size": 276400.0, "url": {"label": "19_0006.pdf", "url": "https://niigata-u.repo.nii.ac.jp/record/2263/files/19_0006.pdf"}, "version_id": "02b16e73-98e0-4782-902a-6f1df5ea733e"}]}, "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": "Critical behavior near the metal-insulator transition in the one-dimensional extended Hubbard model at quarter filling", "item_titles": {"attribute_name": "\u30bf\u30a4\u30c8\u30eb", "attribute_value_mlt": [{"subitem_title": "Critical behavior near the metal-insulator transition in the one-dimensional extended Hubbard model at quarter filling"}, {"subitem_title": "Critical behavior near the metal-insulator transition in the one-dimensional extended Hubbard model at quarter filling", "subitem_title_language": "en"}]}, "item_type_id": "5", "owner": "1", "path": ["453/454", "176/488/489"], "permalink_uri": "http://hdl.handle.net/10191/1151", "pubdate": {"attribute_name": "\u516c\u958b\u65e5", "attribute_value": "2007-04-23"}, "publish_date": "2007-04-23", "publish_status": "0", "recid": "2263", "relation": {}, "relation_version_is_last": true, "title": ["Critical behavior near the metal-insulator transition in the one-dimensional extended Hubbard model at quarter filling"], "weko_shared_id": null}