{"@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/1361699994880197248.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevd.80.054502"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevD.80.054502"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.80.054502/fulltext"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.0905.0962"}}],"dc:title":[{"@value":"SU(2) and SU(3) chiral perturbation theory analyses on baryon masses 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"}],"description":[{"notation":[{"@value":"We investigate the quark mass dependence of baryon masses in 2+1 flavor lattice QCD using SU(3) heavy baryon chiral perturbation theory up to one-loop order. The baryon mass data used for the analyses are obtained for the degenerate up-down quark mass of 3 MeV to 24 MeV and two choices of the strange quark mass around the physical value. We find that the SU(3) chiral expansion fails to describe both the octet and the decuplet baryon data if phenomenological values are employed for the meson-baryon couplings. The SU(2) case is also examined for the nucleon. We observe that higher order terms are controlled only around the physical point. We also evaluate finite size effects using SU(3) heavy baryon chiralperturbation theory, finding small values of order 1% even at the physical point."}]},{"notation":[{"@value":"26 pages, 10 tables, 58 figures"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381699994880197254","@type":"Researcher","foaf:name":[{"@value":"K.-I. Ishikawa"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197248","@type":"Researcher","foaf:name":[{"@value":"N. Ishizuka"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197120","@type":"Researcher","foaf:name":[{"@value":"T. Izubuchi"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197121","@type":"Researcher","foaf:name":[{"@value":"D. Kadoh"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197250","@type":"Researcher","foaf:name":[{"@value":"K. Kanaya"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197256","@type":"Researcher","foaf:name":[{"@value":"Y. Kuramashi"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197253","@type":"Researcher","foaf:name":[{"@value":"Y. Namekawa"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197255","@type":"Researcher","foaf:name":[{"@value":"M. Okawa"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197122","@type":"Researcher","foaf:name":[{"@value":"Y. Taniguchi"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197252","@type":"Researcher","foaf:name":[{"@value":"A. Ukawa"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197249","@type":"Researcher","foaf:name":[{"@value":"N. Ukita"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994880197251","@type":"Researcher","foaf:name":[{"@value":"T. Yoshié"}]}],"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":"2009-09-03","prism:volume":"80","prism:number":"5","prism:startingPage":"054502"},"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.80.054502"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.80.054502/fulltext"}],"createdAt":"2009-09-03","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/1050001202618344960","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Equation of state in 2+1 flavor QCD with improved Wilson quarks by the fixed scale approach"},{"@value":"Equation of state in<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 QCD with improved Wilson quarks by the fixed scale approach"}]},{"@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/1050845760721643264","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Quark scalar, axial, and pseudoscalar charges in the Schwinger-Dyson formalism"}]},{"@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/1360285709977307008","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mi>D</mml:mi></mml:math>meson mass increase by restoration of chiral symmetry in nuclear matter"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861707126152704","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"FLAG Review 2021"}]},{"@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.80.054502"},{"@type":"OPENAIRE","@value":"doi_dedup___::de761c623440bf3138ce203c145f861b"},{"@type":"CROSSREF","@value":"10.1103/physrevd.81.074503_references_DOI_DtE2MDKrk9jNYfustr3EQRyYViC"},{"@type":"CROSSREF","@value":"10.1103/physrevd.85.094508_references_DOI_DtE2MDKrk9jNYfustr3EQRyYViC"},{"@type":"CROSSREF","@value":"10.1140/epjc/s10052-019-7354-7_references_DOI_DtE2MDKrk9jNYfustr3EQRyYViC"},{"@type":"CROSSREF","@value":"10.1103/physrevc.93.045209_references_DOI_DtE2MDKrk9jNYfustr3EQRyYViC"},{"@type":"CROSSREF","@value":"10.1093/ptep/pts002_references_DOI_DtE2MDKrk9jNYfustr3EQRyYViC"},{"@type":"CROSSREF","@value":"10.1103/physrevd.89.074017_references_DOI_DtE2MDKrk9jNYfustr3EQRyYViC"},{"@type":"CROSSREF","@value":"10.1140/epjc/s10052-022-10536-1_references_DOI_DtE2MDKrk9jNYfustr3EQRyYViC"}]}