{"_buckets": {"deposit": "789f4c4c-05c5-477c-86e6-f3f10da35ab4"}, "_deposit": {"id": "2341", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "2341"}, "status": "published"}, "_oai": {"id": "oai:niigata-u.repo.nii.ac.jp:00002341"}, "item_5_biblio_info_6": {"attribute_name": "\u66f8\u8a8c\u60c5\u5831", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2003-07", "bibliographicIssueDateType": "Issued"}, "bibliographicIssueNumber": "1", "bibliographicPageStart": "014501", "bibliographicVolumeNumber": "68", "bibliographic_titles": [{"bibliographic_title": "Physical Review D"}, {"bibliographic_title": "Physical Review D", "bibliographic_titleLang": "en"}]}]}, "item_5_description_4": {"attribute_name": "\u6284\u9332", "attribute_value_mlt": [{"subitem_description": "We explore the application of the domain wall fermion formalism of lattice QCD to calculate the K \u20d7 \u03c0\u03c0 decay amplitudes in terms of the K + \u2192\u03c0 + and K 0 \u21920 hadronic matrix elements through relations derived in chiral perturbation theory. Numerical simulations are carried out in quenched QCD using the domain-wall fermion action for quarks and a renormalization group-improved gauge action for gluons on a 16 3 \u00d732\u00d716 and 24 3 \u00d732\u00d716 lattice at \u03b2=2.6 corresponding to the lattice spacing 1/a\u22482GeV. Quark loop contractions which appear in Penguin diagrams are calculated by the random noise method, and the \u0394I=1/2 matrix elements which require subtractions with the quark loop contractions are obtained with a statistical accuracy of about 10%. We investigate the chiral properties required of the K + \u2192\u03c0 + matrix elements. Matching the lattice matrix elements to those in the continuum at \u03bc=1/a using the perturbative renormalization factor to one loop order, and running to the scale \u03bc=m c =1.3GeV with the renormalization group for N f =3 flavors, we calculate all the matrix elements needed for the decay amplitudes. With these matrix elements, the \u0394I=3/2 decay amplitude ReA 2 shows a good agreement with experiment after an extrapolation to the chiral limit. The \u0394I=1/2 amplitude ReA 0 , on the other hand, is about 50\u201360 % of the experimental one even after chiral extrapolation. In view of the insufficient enhancement of the \u0394I=1/2 contribution, we employ the experimental values for the real parts of the decay amplitudes in our calculation of \u025b \u2032 /\u025b. The central values of our result indicate that the \u0394I=3/2 contribution is larger than the \u0394I=1/2 contribution so that \u025b \u2032 /\u025b is negative and has a magnitude of order 10 -4 . We discuss in detail possible systematic uncertainties, which seem too large for a definite conclusion on the value of \u025b \u2032 /\u025b.", "subitem_description_type": "Abstract"}]}, "item_5_publisher_7": {"attribute_name": "\u51fa\u7248\u8005", "attribute_value_mlt": [{"subitem_publisher": "American Physical Society"}]}, "item_5_relation_14": {"attribute_name": "DOI", "attribute_value_mlt": [{"subitem_relation_type_id": {"subitem_relation_type_id_text": "info:doi/10.1103/PhysRevD.68.014501", "subitem_relation_type_select": "DOI"}}]}, "item_5_rights_15": {"attribute_name": "\u6a29\u5229", "attribute_value_mlt": [{"subitem_rights": "(C) 2003 American Physical Society"}]}, "item_5_select_19": {"attribute_name": "\u8457\u8005\u7248\u30d5\u30e9\u30b0", "attribute_value_mlt": [{"subitem_select_item": "publisher"}]}, "item_5_source_id_11": {"attribute_name": "\u66f8\u8a8c\u30ec\u30b3\u30fc\u30c9ID", "attribute_value_mlt": [{"subitem_source_identifier": "AA00773624", "subitem_source_identifier_type": "NCID"}]}, "item_5_source_id_9": {"attribute_name": "ISSN", "attribute_value_mlt": [{"subitem_source_identifier": "15507998", "subitem_source_identifier_type": "ISSN"}]}, "item_creator": {"attribute_name": "\u8457\u8005", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "Noaki, J."}], "nameIdentifiers": [{"nameIdentifier": "16019", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Aoki, S."}], "nameIdentifiers": [{"nameIdentifier": "16020", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Aoki, Y."}], "nameIdentifiers": [{"nameIdentifier": "16021", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Burkhalter, R."}], "nameIdentifiers": [{"nameIdentifier": "16022", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Ejiri, S."}], "nameIdentifiers": [{"nameIdentifier": "16023", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Fukugita, M."}], "nameIdentifiers": [{"nameIdentifier": "16024", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Hashimoto, S."}], "nameIdentifiers": [{"nameIdentifier": "16025", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Ishizuka, N."}], "nameIdentifiers": [{"nameIdentifier": "16026", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Iwasaki, Y."}], "nameIdentifiers": [{"nameIdentifier": "16027", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Izubuchi, T."}], "nameIdentifiers": [{"nameIdentifier": "16028", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Kanaya, K."}], "nameIdentifiers": [{"nameIdentifier": "16029", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Kaneko, T."}], "nameIdentifiers": [{"nameIdentifier": "16030", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Kuramashi, Y."}], "nameIdentifiers": [{"nameIdentifier": "16031", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Lesk, V."}], "nameIdentifiers": [{"nameIdentifier": "16032", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Nagai, K.I."}], "nameIdentifiers": [{"nameIdentifier": "16033", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Okawa, M."}], "nameIdentifiers": [{"nameIdentifier": "16034", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Taniguchi, Y."}], "nameIdentifiers": [{"nameIdentifier": "16035", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Ukawa, A."}], "nameIdentifiers": [{"nameIdentifier": "16036", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Yoshie, T."}], "nameIdentifiers": [{"nameIdentifier": "16037", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "CP-PACS, Collaboration"}], "nameIdentifiers": [{"nameIdentifier": "16038", "nameIdentifierScheme": 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"http://purl.org/coar/resource_type/c_6501"}]}, "item_title": "Calculation of Nonleptonic kaon decay amplitudes from K\u03c0 matrix elements in quenched domain-wall QCD", "item_titles": {"attribute_name": "\u30bf\u30a4\u30c8\u30eb", "attribute_value_mlt": [{"subitem_title": "Calculation of Nonleptonic kaon decay amplitudes from K\u03c0 matrix elements in quenched domain-wall QCD"}, {"subitem_title": "Calculation of Nonleptonic kaon decay amplitudes from K\u03c0 matrix elements in quenched domain-wall QCD", "subitem_title_language": "en"}]}, "item_type_id": "5", "owner": "1", "path": ["453/454", "176/488/489"], "permalink_uri": "http://hdl.handle.net/10191/27659", "pubdate": {"attribute_name": "\u516c\u958b\u65e5", "attribute_value": "2014-06-23"}, "publish_date": "2014-06-23", "publish_status": "0", "recid": "2341", "relation": {}, "relation_version_is_last": true, "title": ["Calculation of Nonleptonic kaon decay amplitudes from K\u03c0 matrix elements in quenched domain-wall QCD"], 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