{"@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/1360580236947578112.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/j.physletb.2021.136346"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S0370269321002860?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S0370269321002860?httpAccept=text/plain"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.2010.01608"}}],"dc:title":[{"@value":"Spin hydrodynamics and symmetric energy-momentum tensors – A current induced by the spin vorticity –"}],"description":[{"notation":[{"@value":"We discuss a puzzle in relativistic spin hydrodynamics; in the previous formulation the spin source from the antisymmetric part of the canonical energy-momentum tensor (EMT) is crucial. The Belinfante improved EMT is pseudo-gauge transformed from the canonical EMT and is usually a physically sensible choice especially when gauge fields are coupled as in magnetohydrodynamics, but the Belinfante EMT has no antisymmetric part. We find that pseudo-transformed entropy currents are physically inequivalent in nonequilibrium situations. We also identify a current induced by the spin vorticity read from the Belinfante symmetric EMT."}]},{"notation":[{"@value":"6 pages, no figure"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380580236947578113","@type":"Researcher","foaf:name":[{"@value":"Kenji Fukushima"}]},{"@id":"https://cir.nii.ac.jp/crid/1380580236947578112","@type":"Researcher","foaf:name":[{"@value":"Shi Pu"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"03702693"}],"prism:publicationName":[{"@value":"Physics Letters B"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"2021-06","prism:volume":"817","prism:startingPage":"136346"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/","https://www.elsevier.com/legal/tdmrep-license","http://creativecommons.org/licenses/by/4.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:S0370269321002860?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:S0370269321002860?httpAccept=text/plain"}],"createdAt":"2021-05-07","modifiedAt":"2025-10-07","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-%20Phenomenology","dc:title":"High Energy Physics - Phenomenology"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Phenomenology%20(hep-ph)","dc:title":"High Energy Physics - Phenomenology (hep-ph)"},{"@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=Physics","dc:title":"Physics"},{"@id":"https://cir.nii.ac.jp/all?q=QC1-999","dc:title":"QC1-999"},{"@id":"https://cir.nii.ac.jp/all?q=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360021389825825152","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Spin relaxation rate for baryons in a thermal pion gas"}]},{"@id":"https://cir.nii.ac.jp/crid/1360584339752764032","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Dense nuclear matter equation of state from heavy-ion collisions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869856030385536","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Spin polarization in relativistic heavy-ion collisions"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842061969280","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Gyrohydrodynamics : relativistic spinful fluid with strong vorticity"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1016/j.physletb.2021.136346"},{"@type":"OPENAIRE","@value":"doi_dedup___::266b81152a0b3c155744aca63f9eb7a6"},{"@type":"CROSSREF","@value":"10.1103/physrevc.109.054909_references_DOI_Uv2SipBFPWxV3KM7TzR3ZHfHqDg"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptac091_references_DOI_Uv2SipBFPWxV3KM7TzR3ZHfHqDg"},{"@type":"CROSSREF","@value":"10.1016/j.ppnp.2023.104080_references_DOI_Uv2SipBFPWxV3KM7TzR3ZHfHqDg"},{"@type":"CROSSREF","@value":"10.1142/s0218301324300066_references_DOI_Uv2SipBFPWxV3KM7TzR3ZHfHqDg"}]}