{"@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/1361137044453189760.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1088/1126-6708/2008/10/091"}}],"dc:title":[{"@value":"π© = 6 superconformal Chern-Simons-matter theories, M2-branes and their gravity duals"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381137044453189760","@type":"Researcher","foaf:name":[{"@value":"Ofer Aharony"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137044453189763","@type":"Researcher","foaf:name":[{"@value":"Oren Bergman"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137044453189761","@type":"Researcher","foaf:name":[{"@value":"Daniel Louis Jafferis"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137044453189762","@type":"Researcher","foaf:name":[{"@value":"Juan Maldacena"}]}],"publication":{"publicationIdentifier":[{"@type":"EISSN","@value":"10298479"},{"@type":"PISSN","@value":"https://id.crossref.org/issn/11266708"}],"prism:publicationName":[{"@value":"Journal of High Energy Physics"}],"dc:publisher":[{"@value":"Springer Science and Business Media LLC"}],"prism:publicationDate":"2008-10-23","prism:volume":"2008","prism:number":"10","prism:startingPage":"091","prism:endingPage":"091"},"reviewed":"false","createdAt":"2008-10-24","modifiedAt":"2011-08-22","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050001201680241024","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Toward the construction of the general multi-cut solutions in Chern-Simons matrix models"}]},{"@id":"https://cir.nii.ac.jp/crid/1050001335835673728","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Orientifold ABJM matrix model: chiral projections and worldsheet instantons"}]},{"@id":"https://cir.nii.ac.jp/crid/1050001335841122816","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"A proposal of the gauge theory description of the small Schwarzschild black hole in AdS5 Γ S5"},{"@value":"A proposal of the gauge theory description of the small Schwarzschild black hole in AdS5 Γ S5"}]},{"@id":"https://cir.nii.ac.jp/crid/1050001338926128896","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Probing non-perturbative effects in M-theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1050001338926202880","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Non-perturbative effects and the refined topological string"}]},{"@id":"https://cir.nii.ac.jp/crid/1050282810809309440","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Superconformal Chern-Simons partition functions of affine D-type quiver from Fermi gas"}]},{"@id":"https://cir.nii.ac.jp/crid/1050282810809311616","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Large N behavior of mass deformed ABJM theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1050282810809320192","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Exact instanton expansion of superconformal Chern-Simons theories from topological strings"}]},{"@id":"https://cir.nii.ac.jp/crid/1050282813902914048","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Instanton bound states in ABJM theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1050282814175596544","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Partial Deconfinement"}]},{"@id":"https://cir.nii.ac.jp/crid/1050292706231082752","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Non-perturbative tests of duality cascades in three dimensional supersymmetric gauge theories"}]},{"@id":"https://cir.nii.ac.jp/crid/1050564285789094272","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"SchrΓΆdinger geometries arising from Yang-Baxter deformations"},{"@value":"Schroedinger geometries arising from Yang-Baxter deformations"}]},{"@id":"https://cir.nii.ac.jp/crid/1050564288879623680","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Exact results on ABJ theory and the refined topological string"}]},{"@id":"https://cir.nii.ac.jp/crid/1050564289221262080","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Hyperbolic fracton model, subsystem symmetry, and holography"}]},{"@id":"https://cir.nii.ac.jp/crid/1050566774891567872","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Hyperbolic fracton model, subsystem symmetry, and holography. II. The dual eight-vertex model"}]},{"@id":"https://cir.nii.ac.jp/crid/1050568617144597632","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Instanton corrections of 1/6 BPS Wilson loops in ABJM theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1050845760762733952","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Instanton effects in ABJM theory with general R-charge assignments"}]},{"@id":"https://cir.nii.ac.jp/crid/1050845760771254784","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Anomalous dimensions of higher spin currents in large N CFTs"}]},{"@id":"https://cir.nii.ac.jp/crid/1050845760779409024","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Marginal deformations of 3d supersymmetric U(N) model and broken higher spin symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1050850092172877184","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Wilson loops in 3d N=4 SQCD from Fermi gas"},{"@value":"Wilson loops in 3d N $$ \\mathcal{N} $$ = 4 SQCD from Fermi gas"}]},{"@id":"https://cir.nii.ac.jp/crid/1360002215248087040","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"String theory of the Omega deformation"}]},{"@id":"https://cir.nii.ac.jp/crid/1360002217464469504","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"T-systems andY-systems in integrable systems"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004231120511744","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Symmetry breaking in quantum curves and super Chern-Simons matrix models"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004231121873408","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Light states in Chern-Simons theory coupled to fundamental matter"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004231123645184","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Supersymmetry breaking in a large N gauge theory with gravity dual"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004231127909760","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Thermodynamics of black M-branes from SCFTs"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004231128110848","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Linking loops in ABJM and refined theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004231128907392","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Summing up all genus free energy of ABJM matrix model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004231132883584","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Exact results on the ABJM Fermi gas"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004231135688192","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Dualities in ABJM matrix model from closed string viewpoint"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235012070912","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Large-Nreduction forN=2quiver Chern-Simons theories onS3and localization in matrix models"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235012963456","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"M5-branes in the ABJM theory and the Nahm equation"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235021047552","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Masses of higher spin fields onAdS4and conformal perturbation theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004236175167872","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"NUMERICAL STUDIES OF THE ABJM THEORY FOR ARBITRARY N AT ARBITRARY COUPLING CONSTANT"}]},{"@id":"https://cir.nii.ac.jp/crid/1360005515738643072","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Rectangular W-algebras, extended higher spin gravity and dual coset CFTs"}]},{"@id":"https://cir.nii.ac.jp/crid/1360005515752794112","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Hanany-Witten transition in quantum curves"}]},{"@id":"https://cir.nii.ac.jp/crid/1360005515752867840","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Reflection groups and 3d $$ \\mathcal{N} $$> 6 SCFTs"}]},{"@id":"https://cir.nii.ac.jp/crid/1360013168739129472","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"More on $$ \\mathcal{N} $$ =2 S-folds"}]},{"@id":"https://cir.nii.ac.jp/crid/1360016862125902208","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"3d $$ \\mathcal{N} $$ = 3 generalized Giveon-Kutasov duality"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017282422205952","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"S1 reduction of 4D $$ \\mathcal{N} $$ = 3 SCFTs and squashing independence of ABJM theories"}]},{"@id":"https://cir.nii.ac.jp/crid/1360025430215912448","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"A Scaling Relation, Zm-Type Deconfinement Phases, and Imaginary Chemical Potentials in Finite Temperature Large-N Gauge Theories"}]},{"@id":"https://cir.nii.ac.jp/crid/1360283690226474112","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Exact results for vortex loop operators in 3d supersymmetric theories"}]},{"@id":"https://cir.nii.ac.jp/crid/1360283690227470848","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Aspects of AdS/BCFT"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706095545472","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Instanton effects in ABJM theory from Fermi gas approach"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706095553408","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"3d superconformal indices and isomorphisms of M2-brane theories"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706099138560","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Instanton effects in orientifold ABJM theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706100396928","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"ABJM matrix model and 2D Toda lattice hierarchy"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706101297664","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Orthosymplectic Chern-Simons matrix model and chirality projection"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706102842240","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Two-point functions in ABJM matrix model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706105777024","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Instanton effects in orbifold ABJM theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706111480320","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Integrability of BPS equations in ABJM theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706111563136","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Extended higher spin holography and Grassmannian models"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706113484544","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Semiclassical analysis of M2-brane in AdS4ΓS7/Z k"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706113535616","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"BPS solutions in ABJM theory and maximal super Yang-Mills on R Γ S 2"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285711139373568","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"What lattice theorists can do for superstring/M-theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285711139468672","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"M2- and M5-branes in E11 current algebra formulation of M-theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285711323676800","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Hermitian(Ο΅,Ξ΄)-Freudenthal-Kantor Triple Systems and Certain Applications of*-Generalized Jordan Triple Systems to Field Theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360290617471972864","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Categorical perspective on quantization of Poisson algebra"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298757411093504","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Duality cascades and affine Weyl groups"}]},{"@id":"https://cir.nii.ac.jp/crid/1360302866853887232","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"5d AGT correspondence of supergroup gauge theories from quantum toroidal $$ \\mathfrak{gl} $$1"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567181080687232","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Airy function and 4d quantum gravity"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567181086441216","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"ABJM Wilson loops in arbitrary representations"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567181088157568","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"S 3/Z n partition function and dualities"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567181088324096","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Localization on round sphere revisited"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567181089588864","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Superconformal Chern-Simons theories from del Pezzo geometries"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567182359860736","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Membrane quantum mechanics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184963543296","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Higher-derivative gauge interactions of Bagger-Lambert-Gustavsson theory inN=1superspace"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184967975040","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Dualities from largeNorbifold equivalence in Chern-Simons-matter theories with flavor"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567186116011264","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Hermitian generalized Jordan triple systems and certain applications to field theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567186116137088","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Cubic constraints for the resolvents of the ABJM matrix model and its cousins"}]},{"@id":"https://cir.nii.ac.jp/crid/1360572092518377856","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Quantum mirror map for del Pezzo geometries"}]},{"@id":"https://cir.nii.ac.jp/crid/1360576118794378496","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Fermi gas approach to general rank theories and quantum curves"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580229797796480","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Duality cascades and parallelotopes"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580230578890752","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"On $$ \\mathcal{N} $$ = 4 supersymmetry enhancements in three dimensions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360588380581502592","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Affine symmetries for ABJM partition function and its generalization"}]},{"@id":"https://cir.nii.ac.jp/crid/1360588381057254528","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"ADHM Wilson line defect indices"}]},{"@id":"https://cir.nii.ac.jp/crid/1360588381057323136","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"M2-M5 giant graviton expansions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656052234880","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"ABJ fractional brane from ABJM Wilson loop"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656058249600","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Moduli dynamics as a predictive tool for thermal maximally supersymmetric Yang-Mills at large N"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656059647488","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Instanton effects in rank deformed superconformal Chern-Simons theories from topological strings"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656060322304","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Matrix model from $ \\mathcal{N} = 2 $ orbifold partition function"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656063409280","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"From Maxwell-Chern-Simons theory in AdS 3 towards hydrodynamics in 1 + 1 dimensions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656063529088","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Higher spin AdS3 holography with extended supersymmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656063744256","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Higgs phenomenon for higher spin fields on AdS3"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656063896320","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Exact results for ABJ Wilson loops and open-closed duality"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656064579200","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Flowing from 16 to 32 supercharges"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656065222912","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Partition functions of superconformal Chern-Simons theories from Fermi gas approach"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848658850431872","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Giambelli identity in super Chern-Simons matrix model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659948357376","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"ABJM membrane instanton from a pole cancellation mechanism"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848661091527296","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"A class of Hermitian generalized Jordan triple systems and ChernβSimons gauge theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360853567494209408","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Spectral theories and topological strings on del Pezzo geometries"}]},{"@id":"https://cir.nii.ac.jp/crid/1360857593669261824","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Generalized symmetries and holography in ABJM-type theories"}]},{"@id":"https://cir.nii.ac.jp/crid/1360857593787520640","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Rotating multi-charge spindles and their microstates"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861705588509312","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Confinement/deconfinement transition in the D0-brane matrix model β A signature of M-theory?"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861707114924288","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Dualities and flavored indices of M2-brane SCFTs"}]},{"@id":"https://cir.nii.ac.jp/crid/1360865815669606912","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"40 bilinear relations of q-PainlevΓ© VI from $$ \\mathcal{N} $$ = 4 super Chern-Simons theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360865816802472448","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Simple-Sum Giant Graviton Expansions for Orbifolds and Orientifolds"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869855570280448","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Asymptotic Degeneracies of M2-Brane SCFTs"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869856027793280","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Finiteness and uniqueness of duality cascades in three dimensions for affine quivers"}]},{"@id":"https://cir.nii.ac.jp/crid/2050025942155139712","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Analytic continuation for giant gravitons"}]},{"@id":"https://cir.nii.ac.jp/crid/2050307417113794176","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"The partition function of ABJ theory"}]},{"@id":"https://cir.nii.ac.jp/crid/2050307417114067840","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"The Nambu bracket and M-theory"}]},{"@id":"https://cir.nii.ac.jp/crid/2050307417130006272","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Nambu brackets, Chern-Simons theories, quantum curves and M2-branes"}]},{"@id":"https://cir.nii.ac.jp/crid/2050588892091804672","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Resurgence and Lefschetz thimble in three-dimensional N = 2 supersymmetric Chern-Simons matter theories"}]},{"@id":"https://cir.nii.ac.jp/crid/2051433317020886656","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Exact instanton expansion of the ABJM partition function"}]},{"@id":"https://cir.nii.ac.jp/crid/2051714791997621248","@type":"Article","resourceType":"ε¦θ‘ιθͺθ«ζ(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Prospects of the Nambu bracket"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1088/1126-6708/2008/10/091"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2012)148_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1088/1751-8113/44/10/103001_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2019)210_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2013)097_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2016)059_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2016)063_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2019)159_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2013)100_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2015)030_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2011)001_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2014)148_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2014)168_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2012)020_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2016)096_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptt014_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptw070_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1103/physrevd.85.106003_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1103/physrevd.86.125027_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1103/physrevd.94.026004_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep02(2019)147_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2019)101_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2018)168_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2021)054_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2021)012_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep04(2022)158_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2023)255_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptae130_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep04(2015)180_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2014)137_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2011)043_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2013)158_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2013)159_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2017)032_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2016)034_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2019)145_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep04(2016)132_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep05(2013)054_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep05(2018)181_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep06(2016)068_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2014)091_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2016)125_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2013)002_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2013)038_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2010)012_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2011)048_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptv145_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1142/s0217751x16430065_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1142/s0217751x18500513_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1155/2014/310264_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep06(2018)106_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1063/1.5145262_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep05(2022)132_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2022)157_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep02(2017)012_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2013)168_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2012)122_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2013)103_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2016)156_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2017)089_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptw075_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1103/physrevb.99.155126_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1103/physrevd.83.045003_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1103/physrevd.88.065027_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1142/s0217751x14500717_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1142/s0217751x17500567_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2020)158_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1088/1751-8121/acc2fb_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2023)170_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep05(2024)153_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2024)123_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2024)109_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1088/1751-8121/ab93fe_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2014)079_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2017)047_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep05(2012)121_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep05(2015)022_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2015)047_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2017)003_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2011)015_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2015)054_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2014)118_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2014)158_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2014)163_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2015)164_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2016)132_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2014)164_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1063/1.4978229_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1093/ptep/pty118_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1103/physrevd.92.026003_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1142/s0217732314501569_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1103/physrevb.100.245138_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1016/j.nuclphysb.2014.11.024_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2019)176_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2019)197_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2018)175_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2020)154_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2020)077_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptab049_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2021)182_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep05(2022)096_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptac127_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2022)023_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2023)191_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptae006_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1007/s00220-024-05031-5_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"},{"@type":"CROSSREF","@value":"10.1088/1751-8121/adb54c_references_DOI_5PVhwiZO8uejccTl8OwUW7uHByz"}]}