{"@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/1360004231136809344.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1007/jhep12(2011)020"}},{"identifier":{"@type":"URI","@value":"http://link.springer.com/content/pdf/10.1007/JHEP12(2011)020.pdf"}},{"identifier":{"@type":"URI","@value":"http://link.springer.com/article/10.1007/JHEP12(2011)020/fulltext.html"}},{"identifier":{"@type":"URI","@value":"http://link.springer.com/content/pdf/10.1007/JHEP12(2011)020"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1108.5153"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"Direct test of the gauge-gravity correspondence for Matrix theory correlation functions"}],"description":[{"notation":[{"@value":"We study correlation functions in (0+1)-dimensional maximally supersymmetric U(N) Yang-Mills theory, which was proposed by Banks et al. as a non-perturbative definition of 11-dimensional M-theory in the infinite-momentum frame. We perform first-principle calculations using Monte Carlo simulations, and compare the results against the predictions obtained previously based on the gauge-gravity correspondence from 10 dimensions. After providing a self-contained review on these predictions, we present clear evidence that the predictions in the large-N limit actually hold even at small N such as N=2 and 3. The predicted behavior seems to continue to the far infrared regime, which goes beyond the naive range of validity of the 10D supergravity analysis. This suggests that the correlation functions also contain important information on the M-theory limit."}]},{"notation":[{"@value":"v1: 43 pages, 16 figures. v2, v3: minor corrections"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380004231136808970","@type":"Researcher","foaf:name":[{"@value":"Masanori Hanada"}]},{"@id":"https://cir.nii.ac.jp/crid/1420001326225847552","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"90273218"},{"@type":"NRID","@value":"1000090273218"},{"@type":"NRID","@value":"9000351494549"},{"@type":"NRID","@value":"9000002216317"},{"@type":"NRID","@value":"9000003445737"},{"@type":"NRID","@value":"9000413515531"},{"@type":"NRID","@value":"9000401918488"},{"@type":"NRID","@value":"9000401916389"},{"@type":"NRID","@value":"9000258204191"},{"@type":"NRID","@value":"9000312832235"},{"@type":"NRID","@value":"9000241156474"},{"@type":"NRID","@value":"9000258204196"},{"@type":"NRID","@value":"9000014907262"},{"@type":"NRID","@value":"9000241156479"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/jun_nishimura"}],"foaf:name":[{"@value":"Jun Nishimura"}]},{"@id":"https://cir.nii.ac.jp/crid/1420282801198467584","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"50443594"},{"@type":"NRID","@value":"1000050443594"},{"@type":"NRID","@value":"9000309558598"},{"@type":"NRID","@value":"9000409884513"},{"@type":"NRID","@value":"9000006552906"},{"@type":"NRID","@value":"9000018755466"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/ysekino"}],"foaf:name":[{"@value":"Yasuhiro Sekino"}]},{"@id":"https://cir.nii.ac.jp/crid/1420845751158010880","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"10091521"},{"@type":"NRID","@value":"1000010091521"},{"@type":"CINII_AUTHOR_ID","@value":"DA05352628"},{"@type":"URI","@value":"https://ci.nii.ac.jp/author/DA05352628#entity"},{"@type":"URI","@value":"https://viaf.org/viaf/NII%7CDA05352628"},{"@type":"NRID","@value":"9000003385137"},{"@type":"NRID","@value":"9000351425576"},{"@type":"NRID","@value":"9000409996160"},{"@type":"NRID","@value":"9000006611360"},{"@type":"NRID","@value":"9000401949796"},{"@type":"NRID","@value":"9000401927109"},{"@type":"NRID","@value":"9000401925981"},{"@type":"NRID","@value":"9000401945889"},{"@type":"NRID","@value":"9000401900778"},{"@type":"NRID","@value":"9000414949263"},{"@type":"NRID","@value":"9000413578884"},{"@type":"NRID","@value":"9000401951660"},{"@type":"NRID","@value":"9000401946801"},{"@type":"NRID","@value":"9000397824376"},{"@type":"NRID","@value":"9000401953800"},{"@type":"NRID","@value":"9000408424383"},{"@type":"NRID","@value":"9000401930348"},{"@type":"NRID","@value":"9000390916873"},{"@type":"NRID","@value":"9000018086056"},{"@type":"NRID","@value":"9000364780672"},{"@type":"NRID","@value":"9000401926284"},{"@type":"NRID","@value":"9000351426794"},{"@type":"NRID","@value":"9000345325865"},{"@type":"NRID","@value":"9000401950755"},{"@type":"NRID","@value":"9000351422644"},{"@type":"NRID","@value":"9000401947974"},{"@type":"NRID","@value":"9000401944396"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/read0170688"}],"foaf:name":[{"@value":"Tamiaki Yoneya"}]}],"publication":{"publicationIdentifier":[{"@type":"EISSN","@value":"10298479"}],"prism:publicationName":[{"@value":"Journal of High Energy Physics"}],"dc:publisher":[{"@value":"Springer Science and Business Media LLC"}],"prism:publicationDate":"2011-12","prism:volume":"2011","prism:number":"12","prism:startingPage":"020"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["http://www.springer.com/tdm"],"url":[{"@id":"http://link.springer.com/content/pdf/10.1007/JHEP12(2011)020.pdf"},{"@id":"http://link.springer.com/article/10.1007/JHEP12(2011)020/fulltext.html"},{"@id":"http://link.springer.com/content/pdf/10.1007/JHEP12(2011)020"}],"createdAt":"2011-12-12","modifiedAt":"2019-05-22","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Theory","dc:title":"High Energy Physics - Theory"},{"@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-%20Theory%20(hep-th)","dc:title":"High Energy Physics - Theory (hep-th)"},{"@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"}],"project":[{"@id":"https://cir.nii.ac.jp/crid/1040000782094560128","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"21740216"},{"@type":"JGN","@value":"JP21740216"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-21740216/"}],"notation":[{"@language":"ja","@value":"超弦理論が宇宙とブラックホールの量子論に与える示唆"},{"@language":"en","@value":"Implications of superstring theory for cosmology and black hole physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1040282257010846080","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"20340048"},{"@type":"JGN","@value":"JP20340048"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-20340048/"}],"notation":[{"@language":"ja","@value":"ゲージ重力対応と非摂動的超弦理論の構築"},{"@language":"en","@value":"Gauge-gravity correspondence and the construction of non-perturbative string theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1040282257020701696","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"20540286"},{"@type":"JGN","@value":"JP20540286"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-20540286/"}],"notation":[{"@language":"ja","@value":"ゲージ/重力対応の直接検証及びそれに基づく時空構造の研究"},{"@language":"en","@value":"Direct confirmation of the gauge/gravity correspondence and its application to the studies of the space-time structure"}]}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050282677617228928","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Numerical tests of the gauge/gravity duality conjecture for D0-branes at finite temperature and finite N"},{"@value":"Numerical tests of the gauge/gravity duality conjecture for D0-branes at finite temperature and finite \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>N</mml:mi></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1050282814175596544","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Partial Deconfinement"}]},{"@id":"https://cir.nii.ac.jp/crid/1360002217827433344","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Linear responses of D0-branes via gauge/gravity correspondence"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235036525952","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Deconfinement Phase Transition in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi mathvariant=\"script\">N</mml:mi><mml:mo>=</mml:mo><mml:mn>4</mml:mn></mml:math>Super Yang-Mills Theory on<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>R</mml:mi><mml:mo>×</mml:mo><mml:msup><mml:mi>S</mml:mi><mml:mn>3</mml:mn></mml:msup></mml:math>from Supersymmetric Matrix Quantum Mechanics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235036594176","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Higher Derivative Corrections to Black Hole Thermodynamics from Supersymmetric Matrix Quantum Mechanics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004236175167872","@type":"Article","resourceType":"学術雑誌論文(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/1360011145111048448","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Unity of superstring dualities"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011145198010624","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"PP-wave holography for Dp-brane backgrounds"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285709998676224","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Precision lattice test of the gauge/gravity duality at large \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>N</mml:mi></mml:math>"}]},{"@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/1360292620171080320","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"String theory dynamics in various dimensions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567181085414272","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Phase transitions of a (super) quantum mechanical matrix model with a chemical potential"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184990005248","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Schwarzschild Radius from Monte Carlo Calculation of the Wilson Loop in Supersymmetric Matrix Quantum Mechanics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567185894497280","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Holographic description of a quantum black hole on a computer"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574094713389440","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Perturbative renormalization of lattice $ \\mathcal{N} = 4 $ super Yang-Mills theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574096592199808","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Towards a SDLCQ test of the Maldacena conjecture"}]},{"@id":"https://cir.nii.ac.jp/crid/1360846640179685888","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Covariantized matrix theory for D-particles"}]},{"@id":"https://cir.nii.ac.jp/crid/1360846640180937984","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Monte Carlo studies of the spontaneous rotational symmetry breaking in dimensionally reduced super Yang-Mills models"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656057458176","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Gauged and ungauged: a nonperturbative test"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656062994944","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A practical solution to the sign problem in a matrix model for dynamical compactification"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656065060864","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Direct test of the AdS/CFT correspondence by Monte Carlo studies of $ \\mathcal{N}=4 $ super Yang-Mills theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659967056768","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Monte Carlo Studies of Matrix Theory Correlation Functions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855568960398080","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Black-hole–black-string phase transitions in thermal (1 + 1)-dimensional supersymmetric Yang–Mills theory on a circle"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855569433563520","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Comments on thermodynamics of supersymmetric matrix models"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855570930344576","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"D-Brane Bound States Redux"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137043455079808","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Phases of one dimensional large N gauge theory in a 1/D expansion"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137043896988288","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The factorization method for systems with a complex action. A test in Random Matrix Theory for finite density QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137043912305408","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Testing a novel large-<i>N</i>reduction for 𝒩 = 4 super Yang-Mills theory on<i>R</i>×<i>S</i><sup>3</sup>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137044540998784","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Equations of motion and Galilei invariance in D-particle dynamics"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137045227801984","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Multiple D0-branes in weakly curved backgrounds"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137045791636480","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A euclidean lattice construction of supersymmetric Yang-Mills theories with sixteen supercharges"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137046044563584","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Bound states of strings and p-branes"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520244518144","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Multi-body interactions of D-particles in supergravity and Matrix theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520820149504","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Absence of sign problem in two-dimensional $ \\mathcal{N} = \\left( {2,2} \\right) $ super Yang-Mills on lattice"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418521255671040","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Generalized AdS–CFT correspondence for Matrix theory in the large-N limit"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994191137536","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"On the quantum mechanics of supermembranes"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994504955648","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"First results from simulations of supersymmetric lattices"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994694657408","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Monte Carlo studies of the IIB matrix model at large N"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994729085568","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Testing a Fourier-accelerated hybrid Monte Carlo algorithm"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699996499081344","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Phase structure of matrix quantum mechanics at finite temperature"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468340068480","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"PROGRESS IN FOUR-DIMENSIONAL LATTICE SUPERSYMMETRY"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468968651776","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Space-time uncertainty principle and conformal symmetry in D-particle dynamics"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981469504693888","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Anti de Sitter space and holography"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981469811700992","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Direct evidence for the Maldacena conjecture for <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:mi mathvariant=\"script\">N</mml:mi><mml:mo>=</mml:mo><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>8</mml:mn><mml:mo>,</mml:mo><mml:mn>8</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math> super-Yang–Mills theory in <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si2.gif\" overflow=\"scroll\"><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:math> dimensions"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470458058752","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Strings in flat space and pp waves from Script N = 4 Super Yang Mills"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470780844032","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A Monte-Carlo study of the AdS/CFT correspondence: an exploration of quantum gravity effects"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470862377472","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Gauge theory correlators from non-critical string theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981471034081536","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A proposal of a fine tuning free formulation of 4d $ \\mathcal{N} = 4 $ super Yang-Mills"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262943828488832","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Linearized supergravity from Matrix theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262943921993984","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Nonlattice Simulation for Supersymmetric Gauge Theories in One Dimension"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262944653702272","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Restoration of supersymmetry on the lattice: Two-dimensional <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:mi mathvariant=\"script\">N</mml:mi><mml:mo>=</mml:mo><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>2</mml:mn><mml:mo>,</mml:mo><mml:mn>2</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math> supersymmetric Yang–Mills theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544418601157504","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Matrix string theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544419265627392","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Nonperturbative studies of supersymmetric matrix quantum mechanics with 4 and 8 supercharges at finite temperature"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544419615890816","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Extracting black hole physics from the lattice"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544420393543040","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Black holes and membranes in higher-dimensional theories with dilaton fields"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544420489444992","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"D -Particle Bound States and Generalized Instantons"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544420923330304","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Large <i>N</i> dynamics of dimensionally reduced 4D SU(<i>N</i>) super Yang-Mills theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825893655630336","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Resolving the holography in the plane-wave limit of AdS/CFT correspondence"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825893666283136","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The RHMC algorithm for 2 flavours of dynamical staggered fermions"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825894594050432","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Hybrid Monte Carlo"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825894785535744","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Large<i>N</i>BPS states and emergent quantum gravity"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825894834449280","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"High precision study of the structure of <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:mi>D</mml:mi><mml:mo>=</mml:mo><mml:mn>4</mml:mn></mml:math> supersymmetric Yang–Mills quantum mechanics"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107370311806976","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Holographic reformulation of string theory on AdS5×S5 background in the PP-wave limit"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388844040566400","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Generalized conformal symmetry and oblique AdS-CFT correspondence for matrix theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388844559516416","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"M(atrix) theory: matrix quantum mechanics as a fundamental theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388845374337408","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Supersymmetric deformations of type IIB matrix model as matrix regularization of Script N = 4 SYM"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388845795984128","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Holography of Wilson-loop expectation values with local operator insertions"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388846269277952","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Black strings and p-branes"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388846282618752","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Supercurrents in Matrix theory and the generalized AdS/CFT correspondence"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319481595392","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The large $N$ limit of superconformal field theories and supergravity"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951793578904832","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Large N limit of SYM theories with 16 supercharges from superstrings on Dp-brane backgrounds"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951793935832576","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Worldsheet analysis of gauge/gravity dualities"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951794349756416","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Precision holography for non-conformal branes"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951795216483968","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"From supermembrane to matrix string"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951795274283904","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Some physics of the two-dimensional <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:mi mathvariant=\"script\">N</mml:mi><mml:mo>=</mml:mo><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>2</mml:mn><mml:mo>,</mml:mo><mml:mn>2</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math> supersymmetric Yang–Mills theory: Lattice Monte Carlo study"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951795843412864","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Monte Carlo Studies of Supersymmetric Matrix Quantum Mechanics with Sixteen Supercharges at Finite Temperature"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951796071547904","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Towards lattice simulation of the gauge theory duals to black holes and hot strings"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951796209079680","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Thermal phases of D1-branes on a circle from lattice super Yang-Mills"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951796263694208","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Stringy effect of the holographic correspondence for Dp-brane backgrounds"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233270629018240","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Witten index and threshold bound states of D-branes"}]},{"@id":"https://cir.nii.ac.jp/crid/1390282679136015360","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@language":"en","@value":"String Theory and the Space-Time Uncertainty Principle."}]},{"@id":"https://cir.nii.ac.jp/crid/1520010379987774720","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Holography of two-point functions in the spinning string/spin chain correspondence"},{"@language":"ja-Kana","@value":"Holography of two point functions in the spinning string spin chain correspondence"}]},{"@id":"https://cir.nii.ac.jp/crid/1520854805790978048","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Observing dynamical supersymmetry breaking with Euclidean lattice simulations"},{"@language":"ja-Kana","@value":"Observing dynamical supersymmetry breaking with Euclidean lattice simulations"}]},{"@id":"https://cir.nii.ac.jp/crid/1521980705856488832","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Two-dimensional lattice for four-dimensional N = 4 supersymmetric Yang-Mills"},{"@language":"ja-Kana","@value":"Two dimensional lattice for four dimensional N 4 supersymmetric Yang Mills"}]},{"@id":"https://cir.nii.ac.jp/crid/1523951029825493376","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Holography in the Large-J Limit of AdS/CFT Correspondence and Its Applications"},{"@language":"ja-Kana","@value":"Holography in the Large J Limit of AdS CFT Correspondence and Its Applications"},{"@language":"en","@value":"Holography in the Large-J Limit of AdS/CFT Correspondence and Its Applications(Frontiers of Quantum Physics) :"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842043898496","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"The origin of space-time as seen from matrix model simulations"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1007/jhep12(2011)020"},{"@type":"KAKEN","@value":"PRODUCT-13058540"},{"@type":"KAKEN","@value":"PRODUCT-13058569"},{"@type":"KAKEN","@value":"PRODUCT-12042582"},{"@type":"KAKEN","@value":"PRODUCT-12219072"},{"@type":"OPENAIRE","@value":"doi_dedup___::ba777ffaa2131c99c749d4412f98342f"},{"@type":"CROSSREF","@value":"10.1103/physrevd.88.026020_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2019)145_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1103/physrevd.94.094501_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1142/s0217751x16430065_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2017)071_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1126/science.1250122_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1007/jhep06(2016)058_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2013)009_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1007/jhep05(2012)121_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1007/jhep06(2018)124_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2013)200_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1093/ptep/pts004_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"},{"@type":"CROSSREF","@value":"10.1103/physrevd.94.086010_references_DOI_6Lq7OaTgS3yZeyjjt8izNaobMsX"}]}