{"_buckets": {"deposit": "9c6cd67f-9a34-49a9-9fa1-9c628ff8e7b8"}, "_deposit": {"id": "2328", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "2328"}, "status": "published"}, "_oai": {"id": "oai:niigata-u.repo.nii.ac.jp:00002328"}, "item_5_biblio_info_6": {"attribute_name": "\u66f8\u8a8c\u60c5\u5831", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2005-02", "bibliographicIssueDateType": "Issued"}, "bibliographicIssueNumber": "034001", "bibliographicPageEnd": "11", "bibliographicPageStart": "1", "bibliographicVolumeNumber": "71", "bibliographic_titles": [{"bibliographic_title": "Physical Review D"}, {"bibliographic_title": "Physical Review D", "bibliographic_titleLang": "en"}]}]}, "item_5_description_4": {"attribute_name": "\u6284\u9332", "attribute_value_mlt": [{"subitem_description": "The pentaquark (5Q) baryon is studied in anisotropic quenched lattice QCD with renormalized anisotropy as/at=4 for a high-precision mass measurement. The standard Wilson action at \u03b2=5.75 and the O(a) improved Wilson quark action with \u03ba=0.1210(0.0010)0.1240 are employed on a 123\u00d796 lattice. Contribution of excited states is suppressed by using a smeared source. We investigate both the positive- and negative-parity 5Q baryons with I=0 and spin J=1/2 using a non-NK-type interpolating field. After chiral extrapolation, the lowest positive-parity state is found to have a mass, m5Q=2.25\u2009\u2009GeV, which is much heavier than the experimentally observed \u0398+(1540). The lowest negative-parity 5Q state appears at m5Q=1.75\u2009\u2009GeV, which is near the s-wave NK threshold. To distinguish spatially-localized 5Q resonances from NK-scattering states, we propose a new general method imposing a \u201cHybrid Boundary Condition (HBC),\u201d where the NK threshold is artificially raised without affecting compact five-quark states. The study using the HBC method shows that the negative-parity state observed on the lattice is not a compact 5Q state but an s-wave NK-scattering state.", "subitem_description_type": "Abstract"}]}, "item_5_full_name_3": {"attribute_name": "\u8457\u8005\u5225\u540d", "attribute_value_mlt": [{"nameIdentifiers": [{"nameIdentifier": "14312", "nameIdentifierScheme": "WEKO"}], "names": [{"name": "\u8208\u6cbb, \u6587\u5b50"}]}, {"nameIdentifiers": [{"nameIdentifier": "14313", "nameIdentifierScheme": "WEKO"}], "names": [{"name": "Okiharu, Fumiko"}]}]}, "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/PhysRevD.71.034001", "subitem_relation_type_select": "DOI"}}]}, "item_5_rights_15": {"attribute_name": "\u6a29\u5229", "attribute_value_mlt": [{"subitem_rights": "Copyright(C)2005 The American Physical Society"}]}, "item_5_select_19": {"attribute_name": "\u8457\u8005\u7248\u30d5\u30e9\u30b0", "attribute_value_mlt": [{"subitem_select_item": "publisher"}]}, "item_5_source_id_11": {"attribute_name": "\u66f8\u8a8c\u30ec\u30b3\u30fc\u30c9ID", "attribute_value_mlt": [{"subitem_source_identifier": "AA00773624", "subitem_source_identifier_type": "NCID"}]}, "item_5_source_id_9": {"attribute_name": "ISSN", "attribute_value_mlt": [{"subitem_source_identifier": "15507998", "subitem_source_identifier_type": "ISSN"}]}, "item_creator": {"attribute_name": "\u8457\u8005", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "Ishii, N."}], "nameIdentifiers": [{"nameIdentifier": "14308", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Doi, T."}], "nameIdentifiers": [{"nameIdentifier": "14309", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Iida, H."}], "nameIdentifiers": [{"nameIdentifier": "14310", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Okiharu, F."}], "nameIdentifiers": [{"nameIdentifier": "14311", "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": "71_034001_1-11.pdf", "filesize": [{"value": "191.9 kB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_free", "mimetype": "application/pdf", "size": 191900.0, "url": {"label": "71_034001_1-11.pdf", "url": "https://niigata-u.repo.nii.ac.jp/record/2328/files/71_034001_1-11.pdf"}, "version_id": "e1594fb1-0aa3-4992-b539-b64b9854beb9"}]}, "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": "Pentaquark baryon in anisotropic lattice QCD", "item_titles": {"attribute_name": "\u30bf\u30a4\u30c8\u30eb", "attribute_value_mlt": [{"subitem_title": "Pentaquark baryon in anisotropic lattice QCD"}, {"subitem_title": "Pentaquark baryon in anisotropic lattice QCD", "subitem_title_language": "en"}]}, "item_type_id": "5", "owner": "1", "path": ["453/454", "154/501/502"], "permalink_uri": "http://hdl.handle.net/10191/30869", "pubdate": {"attribute_name": "\u516c\u958b\u65e5", "attribute_value": "2014-12-05"}, "publish_date": "2014-12-05", "publish_status": "0", "recid": "2328", "relation": {}, "relation_version_is_last": true, "title": ["Pentaquark baryon in anisotropic lattice QCD"], "weko_shared_id": null}