{"created":"2021-03-01T07:11:27.749063+00:00","id":32735,"links":{},"metadata":{"_buckets":{"deposit":"7d45a9b5-d191-407f-ab47-1b2ca540bc9e"},"_deposit":{"id":"32735","owners":[],"pid":{"revision_id":0,"type":"depid","value":"32735"},"status":"published"},"_oai":{"id":"oai:tsukuba.repo.nii.ac.jp:00032735","sets":["2871:2873:125","3048:798","3:62:5598:84"]},"author_link":["111171","672","111173","111174","111175"],"control_number":"32735","item_1644910766877":{"attribute_name":"出版タイプ","attribute_value_mlt":[{"subitem_version_resource":"http://purl.org/coar/version/c_970fb48d4fbd8a85","subitem_version_type":"VoR"}]},"item_5_biblio_info_6":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2015-01","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"1","bibliographicPageStart":"14508","bibliographicVolumeNumber":"91","bibliographic_titles":[{"bibliographic_title":"Physical review D","bibliographic_titleLang":"en"}]}]},"item_5_description_4":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"We investigate the critical endpoint of finite temperature phase transition of N_f=3 QCD at zero chemical potential. We employ the renormalization-group improved Iwasaki gauge action and nonperturbatively O(a)-improved Wilson-clover fermion action. The critical endpoint is determined by using the intersection point of kurtosis for the temporal size N_t= 4, 6, 8. Spatial sizes of  N_l= 6–16 (N_t= 4), 10–24 (N_t= 6), and 12–24 (N_t= 8) are employed. We find that N_t=4 is out of the scaling region. Using results for N_t= 6 and 8 and making linear extrapolations in 1=N_t^2, we obtain √(t_0 ) T_E= 0.0988(14)(9), √(t_0 ) m_(PS,E)=0.2274(52)(108), and m_(PS,E)/T_E= 2.302(62)(13), where the first error is statistical error, the second error is systematic error, and m_PS is the pseudoscalar meson mass. If one uses 1/√(t_0 )=1.347(30) GeV, as reported by Borsanyi et al., one finds T_E=133(2)(1)(3) MeV, m_(PS,E)=306(7)(14)(7) MeV, and  m_(PS,E)=m_PS^(phys,sym)=0.745(17)(35)(17), where the third error comes from the error of √(t_0 ) and m_PS^(phys,sym)=√(〖(m〗_π^2+〖2m〗_K^2)/3). Our current estimation of √(t_0 ) m_(PS,E) in the continuum limit is about 25% smaller than the SU(3) symmetric point.","subitem_description_language":"en","subitem_description_type":"Abstract"}]},"item_5_publisher_27":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"American Physical Society","subitem_publisher_language":"en"}]},"item_5_relation_11":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type":"isIdenticalTo","subitem_relation_type_id":{"subitem_relation_type_id_text":"https://doi.org/10.1103/PhysRevD.91.014508","subitem_relation_type_select":"DOI"}}]},"item_5_rights_12":{"attribute_name":"権利","attribute_value_mlt":[{"subitem_rights":"(c) 2015 American Physical Society.","subitem_rights_language":"en"}]},"item_5_source_id_7":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"2470-0010","subitem_source_identifier_type":"PISSN"}]},"item_5_source_id_9":{"attribute_name":"書誌レコードID","attribute_value_mlt":[{"subitem_source_identifier":"AA00773624","subitem_source_identifier_type":"NCID"}]},"item_access_right":{"attribute_name":"アクセス権","attribute_value_mlt":[{"subitem_access_right":"open access","subitem_access_right_uri":"http://purl.org/coar/access_right/c_abf2"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"Jin, Xiao-Yong","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Kuramashi,  Yoshinobu","creatorNameLang":"en"},{"creatorName":"藏増, 嘉伸","creatorNameLang":"ja"},{"creatorName":"クラマシ, ヨシノブ","creatorNameLang":"ja-Kana"}],"nameIdentifiers":[{},{},{}]},{"creatorNames":[{"creatorName":"Nakamura, Yoshifumi","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Takeda, Shinji","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Ukawa, Akira","creatorNameLang":"en"},{"creatorName":"宇川, 彰","creatorNameLang":"ja"}],"nameIdentifiers":[{}]}]},"item_files":{"attribute_name":"ファイル情報","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2015-03-05"}],"displaytype":"detail","filename":"PRD_91-1.pdf","filesize":[{"value":"6.9 MB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"PRD_91-1.pdf","objectType":"fulltext","url":"https://tsukuba.repo.nii.ac.jp/record/32735/files/PRD_91-1.pdf"},"version_id":"48f2e764-c22b-4853-8180-ee9f6d792da6"}]},"item_language":{"attribute_name":"言語","attribute_value_mlt":[{"subitem_language":"eng"}]},"item_resource_type":{"attribute_name":"資源タイプ","attribute_value_mlt":[{"resourcetype":"journal article","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"Critical endpoint of the finite temperature phase transition for three flavor QCD","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Critical endpoint of the finite temperature phase transition for three flavor QCD","subitem_title_language":"en"}]},"item_type_id":"5","owner":"1","path":["84","125","798"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2015-03-05"},"publish_date":"2015-03-05","publish_status":"0","recid":"32735","relation_version_is_last":true,"title":["Critical endpoint of the finite temperature phase transition for three flavor QCD"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2022-08-23T06:15:05.765556+00:00"}