{"created":"2021-03-01T06:17:23.084741+00:00","id":835,"links":{},"metadata":{"_buckets":{"deposit":"738c53da-834a-45ba-9ec7-2ba1b171580b"},"_deposit":{"id":"835","owners":[],"pid":{"revision_id":0,"type":"depid","value":"835"},"status":"published"},"_oai":{"id":"oai:repository.dl.itc.u-tokyo.ac.jp:00000835","sets":["43:65:66","9:10:11"]},"item_2_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2011-05","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"9","bibliographicPageEnd":"16","bibliographicPageStart":"1","bibliographicVolumeNumber":"83","bibliographic_titles":[{"bibliographic_title":"Physical review. Third series. D, Particles and fields"}]}]},"item_2_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"We investigate the parity-broken phase structure for staggered and naive fermions in the Gross-Neveu model as a toy model of QCD. We consider a generalized staggered Gross-Neveu model including two types of four-point interactions. We use generalized mass terms to split the doublers for both staggered and naive fermions. The phase boundaries derived from the gap equations show that the mass splitting of tastes results in an Aoki phase both in the staggered and naive cases. We also discuss the continuum limit of these models and explore taking the chirally symmetric limit by fine-tuning a mass parameter and two-coupling constants. This supports the idea that in lattice QCD we can derive one- or two-flavor staggered fermions by tuning the mass parameter, which are likely to be less expensive than Wilson fermions in QCD simulation.","subitem_description_type":"Abstract"}]},"item_2_publisher_20":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"American Physical Society"}]},"item_2_relation_11":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"info:doi/10.1103/PhysRevD.83.094506","subitem_relation_type_select":"DOI"}}]},"item_2_relation_26":{"attribute_name":"異版である","attribute_value_mlt":[{"subitem_relation_type":"isVersionOf","subitem_relation_type_id":{"subitem_relation_type_id_text":"http://doi.org/10.1103/PhysRevD.83.094506","subitem_relation_type_select":"URI"}}]},"item_2_rights_12":{"attribute_name":"権利","attribute_value_mlt":[{"subitem_rights":"© 2011 American Physical Society"}]},"item_2_source_id_10":{"attribute_name":"書誌レコードID","attribute_value_mlt":[{"subitem_source_identifier":"AA00773624","subitem_source_identifier_type":"NCID"}]},"item_2_source_id_8":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"15507998","subitem_source_identifier_type":"ISSN"}]},"item_2_subject_15":{"attribute_name":"日本十進分類法","attribute_value_mlt":[{"subitem_subject":"421","subitem_subject_scheme":"NDC"}]},"item_2_text_4":{"attribute_name":"著者所属","attribute_value_mlt":[{"subitem_text_value":"Physics Department, Brookhaven National Laboratory"},{"subitem_text_value":"Department of Basic Science, University of Tokyo"},{"subitem_text_value":"Yukawa Institute for Theoretical Physics, Kyoto University"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"Creutz, Michael"}],"nameIdentifiers":[{"nameIdentifier":"3221","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Kimura, Taro"}],"nameIdentifiers":[{"nameIdentifier":"3222","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Misumi, Tatsuhiro"}],"nameIdentifiers":[{"nameIdentifier":"3223","nameIdentifierScheme":"WEKO"}]}]},"item_files":{"attribute_name":"ファイル情報","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2017-05-30"}],"displaytype":"detail","filename":"Kimura_PhysRevD83_094506_2011.pdf","filesize":[{"value":"795.7 kB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"Kimura_PhysRevD83_094506_2011.pdf","url":"https://repository.dl.itc.u-tokyo.ac.jp/record/835/files/Kimura_PhysRevD83_094506_2011.pdf"},"version_id":"9172c7f2-f3e1-4e9f-b1d1-46db270dd5a3"}]},"item_keyword":{"attribute_name":"キーワード","attribute_value_mlt":[{"subitem_subject":"PACS numbers: 11.15.Ha, 11.10.Kk, 11.15.Pg, 11.30.Rd","subitem_subject_scheme":"Other"}]},"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":"Aoki phases in the lattice Gross-Neveu model with flavored mass terms","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Aoki phases in the lattice Gross-Neveu model with flavored mass terms"}]},"item_type_id":"2","owner":"1","path":["11","66"],"pubdate":{"attribute_name":"公開日","attribute_value":"2017-01-06"},"publish_date":"2017-01-06","publish_status":"0","recid":"835","relation_version_is_last":true,"title":["Aoki phases in the lattice Gross-Neveu model with flavored mass terms"],"weko_creator_id":"1","weko_shared_id":null},"updated":"2022-12-19T03:41:56.306478+00:00"}