{"@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/1362262943921993984.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevlett.99.161602"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevLett.99.161602"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevLett.99.161602/fulltext"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.0706.1647"}},{"identifier":{"@type":"PMID","@value":"17995236"}}],"dc:title":[{"@value":"Nonlattice Simulation for Supersymmetric Gauge Theories in One Dimension"}],"description":[{"notation":[{"@value":"Lattice simulation of supersymmetric gauge theories is not straightforward. In some cases the lack of manifest supersymmetry just necessitates cumbersome fine-tuning, but in the worse cases the chiral and/or Majorana nature of fermions makes it difficult to even formulate an appropriate lattice theory. We propose to circumvent all these problems inherent in the lattice approach by adopting a non-lattice approach in the case of one-dimensional supersymmetric gauge theories, which are important in the string/M theory context."}]},{"notation":[{"@value":"REVTeX4, 4 pages, 3 figures"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1382262943921993984","@type":"Researcher","foaf:name":[{"@value":"Masanori Hanada"}]},{"@id":"https://cir.nii.ac.jp/crid/1382262943921993985","@type":"Researcher","foaf:name":[{"@value":"Jun Nishimura"}]},{"@id":"https://cir.nii.ac.jp/crid/1382262943921993986","@type":"Researcher","foaf:name":[{"@value":"Shingo Takeuchi"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00319007"},{"@type":"EISSN","@value":"10797114"},{"@type":"PISSN","@value":"http://id.crossref.org/issn/10797114"}],"prism:publicationName":[{"@value":"Physical Review Letters"}],"dc:publisher":[{"@value":"American Physical Society (APS)"}],"prism:publicationDate":"2007-10-18","prism:volume":"99","prism:number":"16","prism:startingPage":"161602"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["http://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"http://link.aps.org/article/10.1103/PhysRevLett.99.161602"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevLett.99.161602/fulltext"}],"createdAt":"2007-10-18","modifiedAt":"2025-01-02","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"}],"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/1360004231136809344","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Direct test of the gauge-gravity correspondence for Matrix theory correlation functions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235012070912","@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:mi>N</mml:mi></mml:math>reduction for<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi mathvariant=\"script\">N</mml:mi><mml:mo mathvariant=\"bold\">=</mml:mo><mml:mn>2</mml:mn></mml:math>quiver Chern-Simons theories on<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>S</mml:mi><mml:mn>3</mml:mn></mml:msup></mml:math>and localization in matrix models"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235036525952","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"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":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Higher Derivative Corrections to Black Hole Thermodynamics from Supersymmetric Matrix Quantum Mechanics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360025430215912448","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"A Scaling Relation, <i>Zm</i>-Type Deconfinement Phases, and Imaginary Chemical Potentials in Finite Temperature Large-<i>N</i> Gauge Theories"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706107266944","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Quantum M-wave and black 0-brane"}]},{"@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/1360290617498975232","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"1/N correction in holographic Wilson loop from quantum gravity"}]},{"@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/1360567182359769472","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Non-perturbative construction of 2D and 4D supersymmetric Yang–Mills theories with 8 supercharges"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184963618432","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"General approach to the sign problem: Factorization method with multiple observables"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184990005248","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"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/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/1360848656058249600","@type":"Article","resourceType":"学術雑誌論文(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/1360848656062994944","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"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/1360848659333201152","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Warm\n                    <i>p</i>\n                    -soup and near extremal black holes"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659967056768","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Monte Carlo Studies of Matrix Theory Correlation Functions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861707147788032","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Precision test of gauge/gravity duality in D0-brane matrix model at low temperature"}]},{"@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"}]},{"@id":"https://cir.nii.ac.jp/crid/2051433317020802304","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Quantum near-horizon geometry of a black 0-brane"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1103/physrevlett.99.161602"},{"@type":"OPENAIRE","@value":"doi_dedup___::3c50502060d546ed668c878b91e42740"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2011)020_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptu028_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1103/physrevd.85.106003_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1103/physrevlett.102.111601_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1103/physrevlett.102.191602_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptae130_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2014)075_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1103/physrevd.94.094501_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1142/s0217751x16430065_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1016/j.nuclphysb.2011.12.014_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2019)138_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2017)071_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1103/physrevd.83.054504_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1103/physrevlett.102.181602_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1126/science.1250122_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2013)009_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2015)047_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1007/jhep10(2011)126_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2013)200_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1088/0264-9381/31/8/085001_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1093/ptep/pts004_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1103/physrevd.94.086010_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1103/physrevlett.104.151601_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"},{"@type":"CROSSREF","@value":"10.1007/jhep03(2023)071_references_DOI_QWbrmfkm0NoWXXQ0nW3OavHjJ8d"}]}