{"@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/1361699993522975488.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevd.94.114510"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevD.94.114510"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.94.114510/fulltext"}}],"dc:title":[{"@value":"Study of the phase diagram of dense two-color QCD within lattice simulation"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381699993522975489","@type":"Researcher","foaf:name":[{"@value":"V. V. Braguta"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699993522975488","@type":"Researcher","foaf:name":[{"@value":"E.-M. Ilgenfritz"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699993522975492","@type":"Researcher","foaf:name":[{"@value":"A. Yu. Kotov"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699993522975491","@type":"Researcher","foaf:name":[{"@value":"A. V. Molochkov"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699993522975490","@type":"Researcher","foaf:name":[{"@value":"A. A. Nikolaev"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"24700010"},{"@type":"EISSN","@value":"24700029"}],"prism:publicationName":[{"@value":"Physical Review D"}],"dc:publisher":[{"@value":"American Physical Society (APS)"}],"prism:publicationDate":"2016-12-15","prism:volume":"94","prism:number":"11","prism:startingPage":"114510"},"reviewed":"false","dc:rights":["http://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"http://link.aps.org/article/10.1103/PhysRevD.94.114510"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.94.114510/fulltext"}],"createdAt":"2016-12-20","modifiedAt":"2017-06-25","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050001335854780672","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Relating quark confinement and chiral symmetry breaking in QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017279866215424","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Study of two color QCD on large lattices"}]},{"@id":"https://cir.nii.ac.jp/crid/1360021389819344256","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Chemical potential (in)dependence of hadron scatterings in the hadronic phase of QCD-like theories and its applications"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298757405329792","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Probing the hadron mass spectrum in dense two-color QCD with the linear sigma model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360302864802975104","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Axial anomaly effect on the chiral-partner structure of diquarks at high temperature"}]},{"@id":"https://cir.nii.ac.jp/crid/1360306905163631616","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Grassmann tensor renormalization group approach to (1+1)-dimensional two-color lattice QCD at finite density"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580232376617600","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Quantum Chromodynamics, Quark Confinement, and Chiral Symmetry Breaking: A Bridge Between Elementary Particle Physics and Nuclear Physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360853567779566592","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Finite-density massless two-color QCD at the isospin Roberge-Weiss point and the 't Hooft anomaly"}]},{"@id":"https://cir.nii.ac.jp/crid/1360865815698325760","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Mass spectrum of spin-one hadrons in dense two-color QCD: Novel predictions by extended linear sigma model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869855104003584","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Lattice study on finite density QC2D towards zero temperature"}]},{"@id":"https://cir.nii.ac.jp/crid/2050588892091732224","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Classification of sign-problem-free relativistic fermions on the basis of the Majorana positivity"}]},{"@id":"https://cir.nii.ac.jp/crid/2050870367085274496","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Velocity of sound beyond the high-density relativistic limit from lattice simulation of dense two-color QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/2051996266988203776","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Relative scale setting for two-color QCD with Nf=2 Wilson fermions"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1103/physrevd.94.114510"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptx040_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1103/physrevd.105.114505_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1007/jhep02(2024)152_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1088/1361-6471/aa8e2f_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptaa170_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptac137_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1103/physrevd.107.054001_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1103/physrevd.108.014030_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2025)027_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1007/978-981-15-8818-1_22-1_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1103/physrevresearch.2.033253_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1103/physrevd.109.074031_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2024)022_references_DOI_2R5i7V0sm7Chd8K17x9i3BbIAzr"}]}