{"created":"2021-03-01T06:30:38.799092+00:00","id":22846,"links":{},"metadata":{"_buckets":{"deposit":"837814df-27bc-4952-b6ec-8efbadec78c9"},"_deposit":{"id":"22846","owners":[],"pid":{"revision_id":0,"type":"depid","value":"22846"},"status":"published"},"_oai":{"id":"oai:nagoya.repo.nii.ac.jp:00022846","sets":["1924:1925:1926"]},"author_link":["67241","67242","67243"],"item_10_biblio_info_6":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2016-09","bibliographicIssueDateType":"Issued"},"bibliographicPageEnd":"055019","bibliographicPageStart":"055019","bibliographicVolumeNumber":"94","bibliographic_titles":[{"bibliographic_title":"Physical Review D"}]}]},"item_10_description_4":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Motivated by the recent CMS excess in a flavor violating Higgs decay h→μτ as well as the anomaly of muon anomalous magnetic moment (muon g−2), we consider a scenario where both the excess in h→μτ and the anomaly of muon g−2 are explained by the μ−τ flavor violation in a general two Higgs doublet model. We study various processes involving μ and τ, and then discuss the typical predictions and constraints in this scenario. Especially, we find that the prediction of τ→μγ can be within the reach of the Belle II experiment. We also show that the lepton nonuniversality between τ→μνν¯ and τ→eνν¯ can be sizable, and hence the analysis of the current Belle data and the future experimental improvement would have an impact on this model. Besides, processes such as τ→μl+l− (l=e,μ), τ→μη, μ→eγ, μ→3e, and the muon electric dipole moment can be accessible, depending on the unknown Yukawa couplings. On the other hand, the processes like τ→eγ and τ→el+l− (l=e,μ) could not be sizable to observe because of the current strong constraints on the e−μ and e−τ flavor violations. Then we also conclude that contrary to the h→μτ decay mode, the lepton flavor violating Higgs boson decay modes h→eμ and h→eτ are strongly suppressed, and hence it will be difficult to observe these modes at the LHC experiment.","subitem_description_language":"en","subitem_description_type":"Abstract"}]},"item_10_identifier_60":{"attribute_name":"URI","attribute_value_mlt":[{"subitem_identifier_type":"DOI","subitem_identifier_uri":"http://doi.org/10.1103/PhysRevD.94.055019"},{"subitem_identifier_type":"HDL","subitem_identifier_uri":"http://hdl.handle.net/2237/25007"}]},"item_10_publisher_32":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"American Physical Society","subitem_publisher_language":"en"}]},"item_10_relation_11":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type":"isVersionOf","subitem_relation_type_id":{"subitem_relation_type_id_text":"https://doi.org/10.1103/PhysRevD.94.055019","subitem_relation_type_select":"DOI"}}]},"item_10_rights_12":{"attribute_name":"権利","attribute_value_mlt":[{"subitem_rights":"© 2016 American Physical Society","subitem_rights_language":"en"}]},"item_10_select_15":{"attribute_name":"著者版フラグ","attribute_value_mlt":[{"subitem_select_item":"publisher"}]},"item_10_source_id_7":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"2470-0029","subitem_source_identifier_type":"PISSN"}]},"item_1615787544753":{"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_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":"Omura, Yuji","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"67241","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Senaha, Eibun","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"67242","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Tobe, Kazuhiro","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"67243","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":"2018-02-22"}],"displaytype":"detail","filename":"PhysRevD_94_055019.pdf","filesize":[{"value":"798.0 kB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"PhysRevD_94_055019.pdf","objectType":"fulltext","url":"https://nagoya.repo.nii.ac.jp/record/22846/files/PhysRevD_94_055019.pdf"},"version_id":"f65d1c3c-a66e-4815-9fee-7005a7c804fd"}]},"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":"τ- and μ-physics in a general two Higgs doublet model with μ−τ flavor violation","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"τ- and μ-physics in a general two Higgs doublet model with μ−τ flavor violation","subitem_title_language":"en"}]},"item_type_id":"10","owner":"1","path":["1926"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2016-11-07"},"publish_date":"2016-11-07","publish_status":"0","recid":"22846","relation_version_is_last":true,"title":["τ- and μ-physics in a general two Higgs doublet model with μ−τ flavor violation"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-01-16T04:50:23.191662+00:00"}