{"@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/1362262944077401600.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevd.73.014511"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevD.73.014511"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.73.014511/fulltext"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.hep-lat/0509049"}}],"dc:title":[{"@value":"Pseudoscalar meson masses in Wilson chiral perturbation theory for<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>flavors"}],"description":[{"notation":[{"@value":"We consider 2+1 flavor Wilson Chiral Perturbation Theory including the lattice spacing contributions of O($a^{2}$). We adopt a power counting appropriate for the unquenched lattice simulations carried out by the CP-PACS/JLQCD collaboration and compute the pseudo scalar meson masses to one loop. These expression are required to perform the chiral extrapolation of the CP-PACS/JLQCD lattice data."}]},{"notation":[{"@value":"18 pages"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1382262944077401602","@type":"Researcher","foaf:name":[{"@value":"S. Aoki"}]},{"@id":"https://cir.nii.ac.jp/crid/1382262944077401601","@type":"Researcher","foaf:name":[{"@value":"O. Bär"}]},{"@id":"https://cir.nii.ac.jp/crid/1382262944077401603","@type":"Researcher","foaf:name":[{"@value":"T. Ishikawa"}]},{"@id":"https://cir.nii.ac.jp/crid/1382262944077401600","@type":"Researcher","foaf:name":[{"@value":"S. Takeda"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"15507998"},{"@type":"EISSN","@value":"15502368"}],"prism:publicationName":[{"@value":"Physical Review D"}],"dc:publisher":[{"@value":"American Physical Society (APS)"}],"prism:publicationDate":"2006-01-18","prism:volume":"73","prism:number":"1","prism:startingPage":"014511"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["http://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"http://link.aps.org/article/10.1103/PhysRevD.73.014511"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.73.014511/fulltext"}],"createdAt":"2006-01-23","modifiedAt":"2017-04-05","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"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050282677624259456","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Scattering lengths for two pseudoscalar meson systems"}]},{"@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":"10.1103/physrevd.73.014511"},{"@type":"OPENAIRE","@value":"doi_dedup___::c8a3f4bcfc47ef7f26c25fd3dd528a6d"},{"@type":"CROSSREF","@value":"10.1103/physrevd.89.054502_references_DOI_CXhnCUPdyrADPh0cgqKD3vCYMJY"},{"@type":"CROSSREF","@value":"10.1093/ptep/pts002_references_DOI_CXhnCUPdyrADPh0cgqKD3vCYMJY"}]}