{"@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/1050292351004475136.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"HDL","@value":"http://hdl.handle.net/2241/0002003921"}},{"identifier":{"@type":"URI","@value":"https://tsukuba.repo.nii.ac.jp/records/2003921"}},{"identifier":{"@type":"DOI","@value":"10.1007/jhep09(2020)177"}},{"identifier":{"@type":"URI","@value":"https://link.springer.com/content/pdf/10.1007/JHEP09(2020)177.pdf"}},{"identifier":{"@type":"URI","@value":"https://link.springer.com/article/10.1007/JHEP09(2020)177/fulltext.html"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.2005.04645"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@language":"en","@value":"Tensor renormalization group approach to four-dimensional complex ?4 theory at finite density"},{"@value":"Tensor renormalization group approach to four-dimensional complex ϕ4 theory at finite density"}],"dc:language":"en","description":[{"type":"abstract","notation":[{"@value":"<jats:title>A<jats:sc>bstract</jats:sc>\n                     </jats:title><jats:p>Tensor network is an attractive approach to the field theory with negative sign problem. The complex <jats:italic>ϕ</jats:italic><jats:sup>4</jats:sup> theory at finite density is a test bed for numerical algorithms to verify their effectiveness. The model shows a characteristic feature called the Silver Blaze phenomenon associated with the sign problem in the large volume limit at low temperature. We analyze the four-dimensional model employing the anisotropic tensor renormalization group algorithm with a parallel computation. We find a clear signal of the Silver Blaze phenomenon on a large volume of <jats:italic>V</jats:italic> = 1024<jats:sup>4</jats:sup>, which implies that the tensor network approach is effective even for four-dimensional field theory beyond two dimensions.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1070019855622545410","@type":"Researcher","foaf:name":[{"@language":"en","@value":"Akiyama Shinichiro"}]},{"@id":"https://cir.nii.ac.jp/crid/1070019855622545408","@type":"Researcher","foaf:name":[{"@language":"en","@value":"Kadoh Daisuke"}]},{"@id":"https://cir.nii.ac.jp/crid/1420001326219182976","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"30280506"},{"@type":"NRID","@value":"1000030280506"},{"@type":"ORCID","@value":"0000-0002-3734-0194"},{"@type":"NRID","@value":"9000413499160"},{"@type":"NRID","@value":"9000006511743"},{"@type":"NRID","@value":"9000413504950"},{"@type":"NRID","@value":"9000413504947"},{"@type":"NRID","@value":"9000239869821"},{"@type":"NRID","@value":"9000255728057"},{"@type":"NRID","@value":"9000006900212"},{"@type":"NRID","@value":"9000241164343"},{"@type":"NRID","@value":"9000401944977"},{"@type":"NRID","@value":"9000399575320"},{"@type":"NRID","@value":"9000267780359"},{"@type":"NRID","@value":"9000413505649"},{"@type":"NRID","@value":"9000413505652"},{"@type":"NRID","@value":"9000022096798"},{"@type":"NRID","@value":"9000241156415"},{"@type":"NRID","@value":"9000287145133"},{"@type":"NRID","@value":"9000413503319"},{"@type":"NRID","@value":"9000239559530"},{"@type":"NRID","@value":"9000402478596"},{"@type":"NRID","@value":"9000392104267"},{"@type":"NRID","@value":"9000413534151"},{"@type":"NRID","@value":"9000413504923"},{"@type":"NRID","@value":"9000413504925"},{"@type":"NRID","@value":"9000019229098"},{"@type":"NRID","@value":"9000014655357"},{"@type":"NRID","@value":"9000241168934"},{"@type":"NRID","@value":"9000021195622"},{"@type":"NRID","@value":"9000402478020"},{"@type":"NRID","@value":"9000413503347"},{"@type":"NRID","@value":"9000413506067"},{"@type":"NRID","@value":"9000413506069"},{"@type":"NRID","@value":"9000413500011"},{"@type":"NRID","@value":"9000413499154"},{"@type":"NRID","@value":"9000287170476"},{"@type":"NRID","@value":"9000003446253"},{"@type":"NRID","@value":"9000241174840"},{"@type":"NRID","@value":"9000267780422"},{"@type":"NRID","@value":"9000413499133"},{"@type":"NRID","@value":"9000413523999"},{"@type":"NRID","@value":"9000413523997"},{"@type":"NRID","@value":"9000392110745"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/read0096954"}],"foaf:name":[{"@language":"en","@value":"Kuramashi Yoshinobu"}]},{"@id":"https://cir.nii.ac.jp/crid/1070019855622545409","@type":"Researcher","foaf:name":[{"@language":"en","@value":"Yamashita Takumi"}]},{"@id":"https://cir.nii.ac.jp/crid/1070019855622545412","@type":"Researcher","foaf:name":[{"@language":"en","@value":"Yoshimura Yusuke"}]}],"publication":{"publicationIdentifier":[{"@type":"EISSN","@value":"10298479"},{"@type":"NCID","@value":"AA1188279X"}],"prism:publicationName":[{"@language":"en","@value":"Journal of High Energy Physics"}],"dc:publisher":[{"@value":"Springer"}],"prism:publicationDate":"2020-09","prism:volume":"2020","prism:number":"9","prism:startingPage":"177"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["Open Access,  © The Authors. Article funded by SCOAP3.","This article is distributed under the terms of the Creative Commons Attribution License (CC-BY 4.0), which permits any use, distribution and reproduction in any medium, provided the original author(s) and source are credited."],"url":[{"@id":"https://tsukuba.repo.nii.ac.jp/records/2003921"},{"@id":"https://link.springer.com/content/pdf/10.1007/JHEP09(2020)177.pdf"},{"@id":"https://link.springer.com/article/10.1007/JHEP09(2020)177/fulltext.html"}],"foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=Lattice%20Quantum%20Field%20Theory","dc:title":"Lattice Quantum Field 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=Nuclear%20and%20particle%20physics.%20Atomic%20energy.%20Radioactivity","dc:title":"Nuclear and particle physics. Atomic energy. Radioactivity"},{"@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"},{"@id":"https://cir.nii.ac.jp/all?q=Field%20Theories%20in%20Higher%20Dimensions","dc:title":"Field Theories in Higher Dimensions"},{"@id":"https://cir.nii.ac.jp/all?q=QC770-798","dc:title":"QC770-798"}],"project":[{"@id":"https://cir.nii.ac.jp/crid/1040848250647653248","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"20H00148"},{"@type":"JGN","@value":"JP20H00148"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-20H00148/"}],"notation":[{"@language":"ja","@value":"テンソルネットワーク法による計算物理学の新展開"},{"@language":"en","@value":"New Development of Computational Physics with Tensor Network 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field"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544420761910656","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Critical behavior of the lattice Schwinger model with a topological term at<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>θ</mml:mi><mml:mo>=</mml:mo><mml:mi>π</mml:mi></mml:mrow></mml:math>using the Grassmann tensor renormalization group"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107368842924544","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Phase transition of four-dimensional Ising model with tensor network scheme"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107369065651328","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"TENSOR RENORMALIZATION GROUP APPROACH TO A LATTICE BOSON 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