{"created":"2021-03-01T07:26:10.408917+00:00","id":46266,"links":{},"metadata":{"_buckets":{"deposit":"8f109b26-0339-4d9d-b3bf-8d0e8dd547d3"},"_deposit":{"id":"46266","owners":[],"pid":{"revision_id":0,"type":"depid","value":"46266"},"status":"published"},"_oai":{"id":"oai:tsukuba.repo.nii.ac.jp:00046266","sets":["117:1206","117:5005","117:5006","117:789","117:790","3:62:5598:84"]},"author_link":["201364","365","188326","203674","270","128757","188319","188320","188321","188322","188323"],"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":"2018-02","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"3","bibliographicPageStart":"032003","bibliographicVolumeNumber":"97","bibliographic_titles":[{"bibliographic_title":"Physical review D","bibliographic_titleLang":"en"}]}]},"item_5_creator_3":{"attribute_name":"著者別名","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"原, 和彦","creatorNameLang":"ja"}],"nameIdentifiers":[{},{},{}]},{"creatorNames":[{"creatorName":"金, 信弘","creatorNameLang":"ja"}],"nameIdentifiers":[{},{},{}]},{"creatorNames":[{"creatorName":"大川, 英希","creatorNameLang":"ja"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"佐藤, 構二","creatorNameLang":"ja"}],"nameIdentifiers":[{},{},{}]},{"creatorNames":[{"creatorName":"受川, 史彦","creatorNameLang":"ja"}],"nameIdentifiers":[{},{},{}]}]},"item_5_description_4":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"A search is presented for the direct pair production of the stop, the supersymmetric partner of the top quark, that decays through an R-parity-violating coupling to a final state with two leptons and two jets, at least one of which is identified as a b-jet. The data set corresponds to an integrated luminosity of 36.1??fb?1 of proton-proton collisions at a center-of-mass energy of √s=13??TeV, collected in 2015 and 2016 by the ATLAS detector at the LHC. No significant excess is observed over the Standard Model background, and exclusion limits are set on stop pair production at a 95% confidence level. Lower limits on the stop mass are set between 600 GeV and 1.5 TeV for branching ratios above 10% for decays to an electron or muon and a b-quark.","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.97.032003","subitem_relation_type_select":"DOI"}}]},"item_5_rights_12":{"attribute_name":"権利","attribute_value_mlt":[{"subitem_rights":"c 2018 CERN, for the ATLAS Collaboration","subitem_rights_language":"en"},{"subitem_rights":"Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.","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":"ATLA Collaboration","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Hara, K.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"\"Ki, , S.H.\"","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"\"Okaw, , H.\"","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Sato, K. ","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Ukegawa, F.","creatorNameLang":"en"}],"nameIdentifiers":[{}]}]},"item_files":{"attribute_name":"ファイル情報","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2018-05-01"}],"displaytype":"detail","filename":"PRD_97-3-032003.pdf","filesize":[{"value":"1.1 MB"}],"format":"application/pdf","licensetype":"license_6","mimetype":"application/pdf","url":{"label":"PRD_97-3-032003","objectType":"fulltext","url":"https://tsukuba.repo.nii.ac.jp/record/46266/files/PRD_97-3-032003.pdf"},"version_id":"5990b1ee-b3b1-4102-afb6-89c880967479"}]},"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":"Search for B?L R-parity-violating top squarks in √s=13??TeV pp collisions with the ATLAS experiment","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Search for B?L R-parity-violating top squarks in √s=13??TeV pp collisions with the ATLAS experiment","subitem_title_language":"en"}]},"item_type_id":"5","owner":"1","path":["790","5005","1206","5006","789","84"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2018-05-01"},"publish_date":"2018-05-01","publish_status":"0","recid":"46266","relation_version_is_last":true,"title":["Search for B?L R-parity-violating top squarks in √s=13??TeV pp collisions with the ATLAS experiment"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-12-21T07:58:56.289626+00:00"}