{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1361137046126914944.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1088/1126-6708/2007/04/092"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.hep-lat/0703006"}}],"dc:title":[{"@value":"Non-perturbative improvement of the axial current with three dynamical flavors and the Iwasaki gauge action"}],"description":[{"notation":[{"@value":"We perform a non-perturbative determination of the improvement coefficient c_A to remove O(a) discretization errors in the axial vector current in three-flavor lattice QCD with the Iwasaki gauge action and the standard O$(a)$-improved Wilson quark action. An improvement condition with a good sensitivity to c_A is imposed at constant physics. Combining our results with the perturbative expansion, c_A is now known rather precisely for 1/a \\gtrsim 1.6 GeV."}]},{"notation":[{"@value":"13 pages, 3 figures, 4 tables"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381137046126914945","@type":"Researcher","foaf:name":[{"@value":"Takashi Kaneko"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137046126914948","@type":"Researcher","foaf:name":[{"@value":"Sinya Aoki"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137046126914947","@type":"Researcher","foaf:name":[{"@value":"Michele Della Morte"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137046126914949","@type":"Researcher","foaf:name":[{"@value":"Shoji Hashimoto"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137046126914944","@type":"Researcher","foaf:name":[{"@value":"Roland Hoffmann"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137046126914946","@type":"Researcher","foaf:name":[{"@value":"Rainer Sommer"}]}],"publication":{"publicationIdentifier":[{"@type":"EISSN","@value":"10298479"}],"prism:publicationName":[{"@value":"Journal of High Energy Physics"}],"dc:publisher":[{"@value":"Springer Science and Business Media LLC"}],"prism:publicationDate":"2007-04-30","prism:volume":"2007","prism:number":"04","prism:startingPage":"092","prism:endingPage":"092"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","createdAt":"2007-05-01","modifiedAt":"2019-01-29","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Lattice","dc:title":"High Energy Physics - Lattice"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Lattice%20(hep-lat)","dc:title":"High Energy Physics - Lattice (hep-lat)"},{"@id":"https://cir.nii.ac.jp/all?q=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"},{"@id":"https://cir.nii.ac.jp/all?q=info:eu-repo/classification/ddc/530","dc:title":"info:eu-repo/classification/ddc/530"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050001335851866880","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Review of lattice results concerning low-energy particle physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1050285299940253312","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"FLAG Review 2019"},{"@value":"FLAG Review 2019: Flavour Lattice Averaging Group (FLAG)"}]},{"@id":"https://cir.nii.ac.jp/crid/1360002218564383104","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Review of lattice results concerning low-energy particle physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235009489280","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Physical point simulation in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mn>2</mml:mn><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:math>flavor lattice QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235011102336","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Charm quark system at the physical point of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mn>2</mml:mn><mml:mo mathvariant=\"bold\">+</mml:mo><mml:mn>1</mml:mn></mml:math>flavor lattice QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656059033472","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Non-perturbative renormalization of quark mass in N f = 2 + 1 QCD with the Schrödinger functional scheme"}]},{"@id":"https://cir.nii.ac.jp/crid/2050307417113766656","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Lattice quantum chromodynamics at the physical point and beyond"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1088/1126-6708/2007/04/092"},{"@type":"OPENAIRE","@value":"doi_dedup___::6eab2014ab74e932724eee5c5e90a969"},{"@type":"CROSSREF","@value":"10.1140/epjc/s10052-014-2890-7_references_DOI_8hurFzVR1tBX4U1knVCVuA71nM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.81.074503_references_DOI_8hurFzVR1tBX4U1knVCVuA71nM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.84.074505_references_DOI_8hurFzVR1tBX4U1knVCVuA71nM"},{"@type":"CROSSREF","@value":"10.1140/epjc/s10052-019-7354-7_references_DOI_8hurFzVR1tBX4U1knVCVuA71nM"},{"@type":"CROSSREF","@value":"10.1140/epjc/s10052-016-4509-7_references_DOI_8hurFzVR1tBX4U1knVCVuA71nM"},{"@type":"CROSSREF","@value":"10.1093/ptep/pts002_references_DOI_8hurFzVR1tBX4U1knVCVuA71nM"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2010)101_references_DOI_8hurFzVR1tBX4U1knVCVuA71nM"}]}