{"@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/1362825893411600640.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevd.78.065035"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevD.78.065035"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.78.065035/fulltext"}}],"dc:title":[{"@value":"Center-stabilized Yang-Mills theory: Confinement and large<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>N</mml:mi></mml:math>volume independence"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1382825893411600641","@type":"Researcher","foaf:name":[{"@value":"Mithat Ünsal"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825893411600640","@type":"Researcher","foaf:name":[{"@value":"Laurence G. Yaffe"}]}],"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":"2008-09-24","prism:volume":"78","prism:number":"6","prism:startingPage":"065035"},"reviewed":"false","dc:rights":["http://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"http://link.aps.org/article/10.1103/PhysRevD.78.065035"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.78.065035/fulltext"}],"createdAt":"2008-09-24","modifiedAt":"2017-06-18","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050575263285135232","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Semiclassics with 't Hooft flux background for QCD with 2-index quarks"}]},{"@id":"https://cir.nii.ac.jp/crid/1050855656184504832","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Center vortex and confinement in Yang–Mills theory and QCD with anomaly-preserving compactifications"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235015557504","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Polyakov loops and the Hosotani mechanism on the lattice"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235023211776","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Phases of circle-compactified QCD with adjoint fermions at finite density"}]},{"@id":"https://cir.nii.ac.jp/crid/1360005517218417280","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Conundrum for the free energy of a holonomous gluonic plasma at cubic order"}]},{"@id":"https://cir.nii.ac.jp/crid/1360009142512895744","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Meson spectrum in the large N limit"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285709990942848","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Large-<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>N</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:math>gauge theory and chiral random matrix theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360302865739835392","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Semiclassical analysis of the bifundamental QCD on ℝ2 × T2 with ’t Hooft flux"}]},{"@id":"https://cir.nii.ac.jp/crid/1360565168533704320","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Volume independence for Yang–Mills fields on the twisted torus"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567182398427648","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Equivalence of large-N gauge theories on a group manifold and its coset space"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184976981504","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Lattice simulations of 10d Yang-Mills toroidally compactified to 1d, 2d, and 4d"}]},{"@id":"https://cir.nii.ac.jp/crid/1360576118701406720","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Exact-WKB, complete resurgent structure, and mixed anomaly in quantum mechanics on S1"}]},{"@id":"https://cir.nii.ac.jp/crid/1360584339772773120","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Winding θ and destructive interference of instantons"}]},{"@id":"https://cir.nii.ac.jp/crid/1360846641058133376","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Polyakov loop modeling for hot QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656051671040","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Phase structure of the twisted SU(3)/U(1)2 flag sigma model on ℝ × S1"}]},{"@id":"https://cir.nii.ac.jp/crid/1360853567488368640","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"From 3D dualities to hadron physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360853567641829760","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Deconfinement and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi mathvariant=\"script\">C</mml:mi><mml:mi mathvariant=\"script\">P</mml:mi></mml:mrow></mml:math>\n breaking at \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>θ</mml:mi><mml:mo>=</mml:mo><mml:mi>π</mml:mi></mml:math>\n in Yang-Mills theories and a novel phase for SU(2)"}]},{"@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/1360865816796942336","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"The large-N limit of the chiral condensate from twisted reduced models"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869854360765056","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Unifying Monopole and Center Vortex as the Semiclassical Confinement Mechanism"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869855555599872","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"The mass of the gluino-glue bound state in large-N $$ \\mathcal{N} $$ = 1 Supersymmetric Yang-Mills theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869856047012864","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Semiclassics for the QCD vacuum structure through T2-compactification with the baryon-’t Hooft flux"}]},{"@id":"https://cir.nii.ac.jp/crid/2050588892101739008","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Infrared renormalon in SU(N) QCD(adj.) on R3×S1"}]},{"@id":"https://cir.nii.ac.jp/crid/2050588892101889408","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Vacuum energy of the supersymmetric CPN-1 model on R×S1 in the 1/N expansion"}]},{"@id":"https://cir.nii.ac.jp/crid/2050588892101895808","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"More on the infrared renormalon in SU (N) QCD(adj.) on R3×S1"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842055154944","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Renormalon structure in compactified spacetime"}]},{"@id":"https://cir.nii.ac.jp/crid/2051433317021890560","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Global inconsistency, 't Hooft anomaly, and level crossing in quantum mechanics"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1103/physrevd.78.065035"},{"@type":"CROSSREF","@value":"10.1103/physrevd.89.094509_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1103/physrevd.96.034022_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptz147_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1007/jhep04(2021)230_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1103/physrevd.88.025046_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptz157_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1007/jhep02(2019)070_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptac042_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2023)146_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1142/s0217751x14450018_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1103/physrevd.96.094502_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1016/j.ppnp.2017.05.002_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptaa066_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2021)096_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2022)038_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2023)033_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptx148_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1103/physrevd.102.125034_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1103/physrevd.102.034020_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1103/physrevresearch.2.033253_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptaa096_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2023)034_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1103/physrevlett.133.171902_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2025)174_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2024)001_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1016/j.physletb.2020.135336_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"},{"@type":"CROSSREF","@value":"10.1016/j.physletb.2018.05.065_references_DOI_7xP0ZZxSXt6qzz15D0IVrmIoKVF"}]}