{"created":"2025-02-21T04:26:00.098735+00:00","id":2008514,"links":{},"metadata":{"_buckets":{"deposit":"0934713b-fbd7-47f4-a68a-67574bc76574"},"_deposit":{"created_by":41,"id":"2008514","owners":[41],"pid":{"revision_id":0,"type":"depid","value":"2008514"},"status":"published"},"_oai":{"id":"oai:hiroshima.repo.nii.ac.jp:02008514","sets":["1730444907710"]},"author_link":[],"item_1617186331708":{"attribute_name":"Title","attribute_value_mlt":[{"subitem_title":"Dynamical quark effects on light quark masses.","subitem_title_language":"en"}]},"item_1617186419668":{"attribute_name":"Creator","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"CP-PACS, Collaboration","creatorNameLang":"en"}],"familyNames":[{"familyName":"CP-PACS","familyNameLang":"en"}],"givenNames":[{"givenName":"Collaboration","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Ali Khan, A","creatorNameLang":"en"}],"familyNames":[{"familyName":"Ali Khan","familyNameLang":"en"}],"givenNames":[{"givenName":"A","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Aoki, S","creatorNameLang":"en"}],"familyNames":[{"familyName":"Aoki","familyNameLang":"en"}],"givenNames":[{"givenName":"S","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Boyd, G","creatorNameLang":"en"}],"familyNames":[{"familyName":"Boyd","familyNameLang":"en"}],"givenNames":[{"givenName":"G","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Burkhalter, R","creatorNameLang":"en"}],"familyNames":[{"familyName":"Burkhalter","familyNameLang":"en"}],"givenNames":[{"givenName":"R","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Ejiri, S","creatorNameLang":"en"}],"familyNames":[{"familyName":"Ejiri","familyNameLang":"en"}],"givenNames":[{"givenName":"S","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Fukugita, M","creatorNameLang":"en"}],"familyNames":[{"familyName":"Fukugita","familyNameLang":"en"}],"givenNames":[{"givenName":"M","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Hashimoto, S","creatorNameLang":"en"}],"familyNames":[{"familyName":"Hashimoto","familyNameLang":"en"}],"givenNames":[{"givenName":"S","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Ishizuka, N","creatorNameLang":"en"}],"familyNames":[{"familyName":"Ishizuka","familyNameLang":"en"}],"givenNames":[{"givenName":"N","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Iwasaki, Y","creatorNameLang":"en"}],"familyNames":[{"familyName":"Iwasaki","familyNameLang":"en"}],"givenNames":[{"givenName":"Y","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Kanaya, K","creatorNameLang":"en"}],"familyNames":[{"familyName":"Kanaya","familyNameLang":"en"}],"givenNames":[{"givenName":"K","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Kaneko, T","creatorNameLang":"en"}],"familyNames":[{"familyName":"Kaneko","familyNameLang":"en"}],"givenNames":[{"givenName":"T","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Kuramashi, Y","creatorNameLang":"en"}],"familyNames":[{"familyName":"Kuramashi","familyNameLang":"en"}],"givenNames":[{"givenName":"Y","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Manke, T","creatorNameLang":"en"}],"familyNames":[{"familyName":"Manke","familyNameLang":"en"}],"givenNames":[{"givenName":"T","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Nagai, K","creatorNameLang":"en"}],"familyNames":[{"familyName":"Nagai","familyNameLang":"en"}],"givenNames":[{"givenName":"K","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Okawa, Masanori","creatorNameLang":"en"}],"familyNames":[{"familyName":"Okawa","familyNameLang":"en"}],"givenNames":[{"givenName":"Masanori","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Shanahan, H. P.","creatorNameLang":"en"}],"familyNames":[{"familyName":"Shanahan","familyNameLang":"en"}],"givenNames":[{"givenName":"H. P.","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Ukawa, A","creatorNameLang":"en"}],"familyNames":[{"familyName":"Ukawa","familyNameLang":"en"}],"givenNames":[{"givenName":"A","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Yoshié, T","creatorNameLang":"en"}],"familyNames":[{"familyName":"Yoshié","familyNameLang":"en"}],"givenNames":[{"givenName":"T","givenNameLang":"en"}]}]},"item_1617186476635":{"attribute_name":"Access Rights","attribute_value_mlt":[{"subitem_access_right":"open access","subitem_access_right_uri":"http://purl.org/coar/access_right/c_abf2"}]},"item_1617186499011":{"attribute_name":"Rights","attribute_value_mlt":[{"subitem_rights":"Copyright (c) 2000 The American Physical Society"}]},"item_1617186609386":{"attribute_name":"Subject","attribute_value_mlt":[{"subitem_subject":"420","subitem_subject_scheme":"Other"}]},"item_1617186626617":{"attribute_name":"Description","attribute_value_mlt":[{"subitem_description":"Light quark masses are calculated in lattice QCD with two degenerate flavors of dynamical quarks. The calculations are made with improved actions with lattice spacing a = 0.22–0.11 fm. In the continuum limit we find mudMS̅(2 GeV) = 3.44-0.22+0.14 MeV using the π and ρ meson masses as physical input, and msMS̅(2 GeV) = 88-6+4 MeV or 90-11+5 MeV with the K or φ meson mass as additional input. The quoted errors represent statistical and systematic combined, the latter including those from continuum and chiral extrapolations, and from renormalization factors. Compared to quenched results, two flavors of dynamical quarks reduce quark masses by about 25%.","subitem_description_language":"en"}]},"item_1617186643794":{"attribute_name":"Publisher","attribute_value_mlt":[{"subitem_publisher":"The American Physical Society"}]},"item_1617186702042":{"attribute_name":"Language","attribute_value_mlt":[{"subitem_language":"eng"}]},"item_1617186920753":{"attribute_name":"Source Identifier","attribute_value_mlt":[{"subitem_source_identifier":"0031-9007","subitem_source_identifier_type":"ISSN"}]},"item_1617187024783":{"attribute_name":"Page Start","attribute_value_mlt":[{"subitem_start_page":"4674"}]},"item_1617187056579":{"attribute_name":"Bibliographic Information","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2000","bibliographicIssueDateType":"Issued"},"bibliographicPageEnd":"4677","bibliographicPageStart":"4674","bibliographicVolumeNumber":"85","bibliographic_titles":[{"bibliographic_title":"Physical Review Letters"},{"bibliographic_title":"Physical Review Letters"}]}]},"item_1617258105262":{"attribute_name":"Resource Type","attribute_value_mlt":[{"resourcetype":"journal article","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_1617265215918":{"attribute_name":"Version Type","attribute_value_mlt":[{"subitem_version_resource":"http://purl.org/coar/version/c_970fb48d4fbd8a85","subitem_version_type":"VoR"}]},"item_1617353299429":{"attribute_name":"Relation","attribute_value_mlt":[{"subitem_relation_type":"isVersionOf","subitem_relation_type_id":{"subitem_relation_type_id_text":"http://dx.doi.org/10.1103/PhysRevLett.85.4674","subitem_relation_type_select":"DOI"}}]},"item_1617605131499":{"attribute_name":"File","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_access","date":[{"dateType":"Available","dateValue":"2023-03-18"}],"displaytype":"simple","filename":"p4674_1.pdf","filesize":[{"value":"98.7 KB"}],"mimetype":"application/pdf","url":{"objectType":"fulltext","url":"https://hiroshima.repo.nii.ac.jp/record/2008514/files/p4674_1.pdf"},"version_id":"201f6a90-468d-458e-b07c-63ae9a768d5d"}]},"item_1732771732025":{"attribute_name":"旧ID","attribute_value":"14502"},"item_title":"Dynamical quark effects on light quark masses.","item_type_id":"40003","owner":"41","path":["1730444907710"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2023-03-18"},"publish_date":"2023-03-18","publish_status":"0","recid":"2008514","relation_version_is_last":true,"title":["Dynamical quark effects on light quark masses."],"weko_creator_id":"41","weko_shared_id":-1},"updated":"2025-02-22T03:50:23.214024+00:00"}