{"@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/1362825893591720320.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevc.82.041303"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevC.82.041303"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevC.82.041303/fulltext"}}],"dc:title":[{"@value":"Enhanced<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>E</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:math>transitions and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>α</mml:mi><mml:mo>+</mml:mo><mml:msup><mml:mi/><mml:mrow><mml:mn>208</mml:mn></mml:mrow></mml:msup><mml:mi mathvariant=\"normal\">Pb</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msup><mml:mn>3</mml:mn><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:math>clustering in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">Po</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>212</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>"}],"description":[{"notation":[{"@value":"We formulate a model for {sup 212}Po, based on the coupled-channels of {alpha}+{sup 208}Pb(0{sup +}) and {alpha}+{sup 208}Pb(3{sup -}) in which the {alpha}-Pb interaction contains scalar, quadrupole, and octupole terms. The model reproduces the recently observed enhanced E1 transitions from the several new negative-parity levels to the yrast states. Because these data are hard to understand in the shell model, this success gives a strong support for a unique role of {alpha}+{sup 208}Pb(3{sup -}) clustering in {sup 212}Po."}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380853567344570125","@type":"Researcher","foaf:name":[{"@value":"Y. Suzuki"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825893591720320","@type":"Researcher","foaf:name":[{"@value":"S. Ohkubo"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"05562813"},{"@type":"EISSN","@value":"1089490X"}],"prism:publicationName":[{"@value":"Physical Review C"}],"dc:publisher":[{"@value":"American Physical Society (APS)"}],"prism:publicationDate":"2010-10-20","prism:volume":"82","prism:number":"4","prism:startingPage":"041303(R)"},"reviewed":"false","dc:rights":["http://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"http://link.aps.org/article/10.1103/PhysRevC.82.041303"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevC.82.041303/fulltext"}],"createdAt":"2010-10-20","modifiedAt":"2017-04-05","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050869456408519040","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Isoscalar dipole transition as a probe for asymmetric clustering"}]},{"@id":"https://cir.nii.ac.jp/crid/1360290617390420992","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Isoscalar transitions in heavy nuclei and α cluster structure"}]},{"@id":"https://cir.nii.ac.jp/crid/1360290617390434560","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Continuum strength of isoscalar transiton of α + <sup>40</sup>Ca in <sup>44</sup>Ti"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659932210560","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Shell-model study of Pb, Bi, Po, At, Rn, and Fr isotopes with masses from 210 to 217"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659932343168","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Bose-Einstein condensation of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mi>α</mml:mi></mml:math>\n clusters and new soft mode in \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>12</mml:mn></mml:mmultiscripts></mml:math>\n–\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi>Fe</mml:mi><mml:mprescripts/><mml:none/><mml:mn>52</mml:mn></mml:mmultiscripts></mml:math>\n \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:mn>4</mml:mn><mml:mi>N</mml:mi></mml:mrow></mml:math>\n nuclei in a field-theoretical superfluid cluster model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360853567344570112","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Isoscalar transitions and $$\\alpha $$ cluster structures in heavy nuclei"}]},{"@id":"https://cir.nii.ac.jp/crid/2051714792013558528","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Existence of core excited 8Be* = α + α* cluster structure in α + α scattering"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1103/physrevc.82.041303"},{"@type":"OPENAIRE","@value":"doi_dedup___::b76fac65b12b8cb9c74e44c4bce10c26"},{"@type":"CROSSREF","@value":"10.1063/5.0037182_references_DOI_Q2YI173CsdBjzbvxYQGaC3BVXKe"},{"@type":"CROSSREF","@value":"10.1080/00223131.2020.1769765_references_DOI_Q2YI173CsdBjzbvxYQGaC3BVXKe"},{"@type":"CROSSREF","@value":"10.1103/physrevc.93.034319_references_DOI_Q2YI173CsdBjzbvxYQGaC3BVXKe"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptab126_references_DOI_Q2YI173CsdBjzbvxYQGaC3BVXKe"},{"@type":"CROSSREF","@value":"10.1103/physrevc.98.014308_references_DOI_Q2YI173CsdBjzbvxYQGaC3BVXKe"},{"@type":"CROSSREF","@value":"10.1103/physrevc.98.044303_references_DOI_Q2YI173CsdBjzbvxYQGaC3BVXKe"},{"@type":"CROSSREF","@value":"10.1140/epja/s10050-021-00372-4_references_DOI_Q2YI173CsdBjzbvxYQGaC3BVXKe"}]}