{"created":"2021-03-01T06:15:12.285493+00:00","id":12295,"links":{},"metadata":{"_buckets":{"deposit":"d7f6477e-6a69-406d-a821-c300042cf72d"},"_deposit":{"id":"12295","owners":[],"pid":{"revision_id":0,"type":"depid","value":"12295"},"status":"published"},"_oai":{"id":"oai:soar-ir.repo.nii.ac.jp:00012295","sets":["1169:1171:1172:1218"]},"author_link":["37335"],"item_10_biblio_info_6":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"1967-03-13","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"1","bibliographicPageEnd":"29","bibliographicPageStart":"25","bibliographicVolumeNumber":"1","bibliographic_titles":[{"bibliographic_title":"信州大学理学部紀要"}]}]},"item_10_description_20":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Transition Processes induced by a weak interaction are formulated by using DEWITT'S method of state vector normalization. It is shown that the transition matrix elements take a form of the product of the scattering matrix element of the final interaction and the matrix element of the weak interaction Hamiltonian between two | φ(1)>-type state vectors. The well-known phases of the transition matrix elements, when the theory is invariant under time reversal, are easily obtained from this form of the S-matrix.","subitem_description_type":"Abstract"}]},"item_10_description_30":{"attribute_name":"資源タイプ（コンテンツの種類）","attribute_value_mlt":[{"subitem_description":"Article","subitem_description_type":"Other"}]},"item_10_description_5":{"attribute_name":"引用","attribute_value_mlt":[{"subitem_description":"信州大学理学部紀要 1(1): 25-29(1967)","subitem_description_type":"Other"}]},"item_10_publisher_4":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"信州大学理学部"}]},"item_10_source_id_35":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"0583-063X","subitem_source_identifier_type":"PISSN"}]},"item_10_source_id_40":{"attribute_name":"書誌レコードID","attribute_value_mlt":[{"subitem_source_identifier":"AA00697923","subitem_source_identifier_type":"NCID"}]},"item_1627890569677":{"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_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"TAKAO,  YASUTARO","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":"2015-09-28"}],"displaytype":"detail","filename":"Science01-01-04.pdf","filesize":[{"value":"131.1 kB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"Science01-01-04.pdf","url":"https://soar-ir.repo.nii.ac.jp/record/12295/files/Science01-01-04.pdf"},"version_id":"914f7fa7-30ac-42d2-9be4-8ec9bda4025a"}]},"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":"departmental bulletin paper","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"State Vector Renormalization in Weak Processes","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"State Vector Renormalization in Weak Processes","subitem_title_language":"en"}]},"item_type_id":"10","owner":"1","path":["1218"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2010-10-06"},"publish_date":"2010-10-06","publish_status":"0","recid":"12295","relation_version_is_last":true,"title":["State Vector Renormalization in Weak Processes"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-03-08T01:36:34.275155+00:00"}