{"@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/1360574093973339776.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevd.86.025022"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/accepted/10.1103/PhysRevD.86.025022"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevD.86.025022"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.86.025022/fulltext"}}],"dc:title":[{"@value":"Solving the 3D Ising model with the conformal bootstrap"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380574093973339776","@type":"Researcher","foaf:name":[{"@value":"Sheer El-Showk"}]},{"@id":"https://cir.nii.ac.jp/crid/1380574093973339780","@type":"Researcher","foaf:name":[{"@value":"Miguel F. Paulos"}]},{"@id":"https://cir.nii.ac.jp/crid/1380574093973339778","@type":"Researcher","foaf:name":[{"@value":"David Poland"}]},{"@id":"https://cir.nii.ac.jp/crid/1380574093973339781","@type":"Researcher","foaf:name":[{"@value":"Slava Rychkov"}]},{"@id":"https://cir.nii.ac.jp/crid/1380574093973339779","@type":"Researcher","foaf:name":[{"@value":"David Simmons-Duffin"}]},{"@id":"https://cir.nii.ac.jp/crid/1380574093973339777","@type":"Researcher","foaf:name":[{"@value":"Alessandro Vichi"}]}],"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":"2012-07-20","prism:volume":"86","prism:number":"2","prism:startingPage":"025022"},"reviewed":"false","dc:rights":["http://link.aps.org/licenses/aps-default-license","http://link.aps.org/licenses/aps-default-accepted-manuscript-license"],"url":[{"@id":"http://link.aps.org/accepted/10.1103/PhysRevD.86.025022"},{"@id":"http://link.aps.org/article/10.1103/PhysRevD.86.025022"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.86.025022/fulltext"}],"createdAt":"2012-07-21","modifiedAt":"2019-07-01","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050001202592548096","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Conformal amplitude hierarchy and the Poincaré disk"}]},{"@id":"https://cir.nii.ac.jp/crid/1050564285816396672","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Three Point Functions in Higher Spin AdS3 Holography with 1/N Corrections"}]},{"@id":"https://cir.nii.ac.jp/crid/1050566774891616640","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Closed-form expression for cross-channel conformal blocks near the lightcone"}]},{"@id":"https://cir.nii.ac.jp/crid/1051975278334813312","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Lightcone expansions of conformal blocks in closed form"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004232439889408","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Five dimensional <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:mi>O</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>N</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:math>-symmetric CFTs from conformal bootstrap"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235015694848","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Approaching the conformal window of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>O</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>n</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>×</mml:mo><mml:mi>O</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>m</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:math>symmetric Landau-Ginzburg models using the conformal bootstrap"}]},{"@id":"https://cir.nii.ac.jp/crid/1360005519986820608","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Conformal blocks from Wilson lines with loop corrections"}]},{"@id":"https://cir.nii.ac.jp/crid/1360013168874697600","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Is there supersymmetric Lee–Yang fixed point in three dimensions?"}]},{"@id":"https://cir.nii.ac.jp/crid/1360025430655775616","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Constraints on the spectrum of field theories with non-integer $O(N)$ symmetry from quantum evanescence"}]},{"@id":"https://cir.nii.ac.jp/crid/1360283693557109376","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Three ways to solve critical ϕ4 theory on 4 − 𝜖 dimensional real projective space: Perturbation, bootstrap, and Schwinger–Dyson equation"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285710024642816","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Surprises in \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>O</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>N</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:math>\n Models: Nonperturbative Fixed Points, Large \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>N</mml:mi></mml:math>\n Limits, and Multicriticality"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285711139373568","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"What lattice theorists can do for superstring/M-theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360302866853862016","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Cosmological phase transitions in composite Higgs models"}]},{"@id":"https://cir.nii.ac.jp/crid/1360306906075902336","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Functional renormalization group approach to dipolar fixed point which is scale invariant but nonconformal"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184941301632","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Functional renormalization group approach to noncollinear magnets"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184970467968","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Bootstrapping phase transitions in QCD and frustrated spin systems"}]},{"@id":"https://cir.nii.ac.jp/crid/1360846643510528512","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Bootstrap experiments on higher dimensional CFTs"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656067173376","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"On the CFT operator spectrum at large global charge"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656323985664","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Fractal Dimensions of Self-Avoiding Walks and Ising High-Temperature Graphs in 3D Conformal Bootstrap"}]},{"@id":"https://cir.nii.ac.jp/crid/1360849944305786624","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Fusion of spin fields in\n                    <i>W</i>\n                    <sub>3</sub>\n                    conformal field theories"}]},{"@id":"https://cir.nii.ac.jp/crid/1360857593806532608","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Recursive structure of the Gauß hypergeometric function and boundary/crosscap conformal block"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869854365728896","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Large landscape of 4d superconformal field theories from small gauge theories"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869855562767232","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Global fixed point potential approach to frustrated antiferromagnets"}]},{"@id":"https://cir.nii.ac.jp/crid/1361131421089607168","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Exclusion inside or at the border of conformal bootstrap continent"}]},{"@id":"https://cir.nii.ac.jp/crid/1361975840580883840","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"autoboot: a generator of bootstrap equations with global symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1520854805481928192","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Renormalisation of parabolic stochastic PDEs"}]},{"@id":"https://cir.nii.ac.jp/crid/2050025942137368064","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"The ε-expansion of the codimension two twist defect from conformal field theory"}]},{"@id":"https://cir.nii.ac.jp/crid/2050870367067486592","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Upper bound on the mass anomalous dimension in many-flavor gauge theories : a conformal bootstrap approach"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1103/physrevd.86.025022"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptw046_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1103/physrevd.89.126009_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.3390/universe3040070_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1103/physrevd.97.086014_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1016/j.physletb.2014.05.058_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1142/s0217751x21501761_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2020)055_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.21468/scipostphyscore.7.3.055_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1142/s0217751x18500495_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1088/1742-6596/965/1/012036_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1103/physrevlett.119.191602_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1142/s0217751x16430065_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2023)053_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1103/physrevd.110.025020_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1103/physrevb.93.064405_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1103/physrevd.91.021901_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1007/jhep06(2019)084_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1007/jhep06(2020)105_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1142/s0217751x18500367_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2015)071_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1007/s10955-016-1658-x_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptw115_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1088/1751-8121/ab56e3_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1142/s0217732321502722_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2024)010_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1088/1742-5468/adacd6_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1142/s0217751x20500360_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"},{"@type":"CROSSREF","@value":"10.1007/s11537-018-1742-x_references_DOI_4mE1uhzjasApKbSvXgBihsaCV1n"}]}