{"@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/1361981468720434560.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevlett.104.042701"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevLett.104.042701"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevLett.104.042701/fulltext"}}],"dc:title":[{"@value":"Novel Manifestation of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>α</mml:mi></mml:math>-Clustering Structures: New “<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>α</mml:mi><mml:mo>+</mml:mo><mml:mmultiscripts><mml:mi>Pb</mml:mi><mml:mprescripts/><mml:none/><mml:mn>208</mml:mn></mml:mmultiscripts></mml:math>” States in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mmultiscripts><mml:mi>Po</mml:mi><mml:mprescripts/><mml:none/><mml:mn>212</mml:mn></mml:mmultiscripts></mml:math>Revealed by Their Enhanced<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>E</mml:mi><mml:mn>1</mml:mn></mml:math>Decays"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380005516079923588","@type":"Researcher","foaf:name":[{"@value":"A. Astier"}]},{"@id":"https://cir.nii.ac.jp/crid/1381981468720434563","@type":"Researcher","foaf:name":[{"@value":"P. Petkov"}]},{"@id":"https://cir.nii.ac.jp/crid/1381981468720434561","@type":"Researcher","foaf:name":[{"@value":"M.-G. Porquet"}]},{"@id":"https://cir.nii.ac.jp/crid/1381981468720434564","@type":"Researcher","foaf:name":[{"@value":"D. S. Delion"}]},{"@id":"https://cir.nii.ac.jp/crid/1381981468720434562","@type":"Researcher","foaf:name":[{"@value":"P. Schuck"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00319007"},{"@type":"EISSN","@value":"10797114"}],"prism:publicationName":[{"@value":"Physical Review Letters"}],"dc:publisher":[{"@value":"American Physical Society (APS)"}],"prism:publicationDate":"2010-01-25","prism:volume":"104","prism:number":"4","prism:startingPage":"042701"},"reviewed":"false","dc:rights":["http://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"http://link.aps.org/article/10.1103/PhysRevLett.104.042701"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevLett.104.042701/fulltext"}],"createdAt":"2010-01-25","modifiedAt":"2025-01-02","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050291768040687744","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Effective interactions between nuclear clusters"}]},{"@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/1360005516079922816","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Nonlocalized clustering and evolution of cluster structure in nuclei"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184955637120","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Octupole phonon model based on the shell model for octupole vibrational states"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567186080858752","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"A revised B(E2;2+ 1 $ \\rightarrow$ → 0+ 1) value in the semi-magic nucleus 210Po"}]},{"@id":"https://cir.nii.ac.jp/crid/1360846642776175104","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Theory and application of explicitly correlated Gaussians"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656394909056","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Alpha-clustering effects in heavy nuclei"}]},{"@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/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/physrevlett.104.042701"},{"@type":"CROSSREF","@value":"10.1007/s11467-019-0917-0_references_DOI_NSeEndFdYBMLwcoCjFmWypsF6Dn"},{"@type":"CROSSREF","@value":"10.1103/physrevc.93.034319_references_DOI_NSeEndFdYBMLwcoCjFmWypsF6Dn"},{"@type":"CROSSREF","@value":"10.1103/physrevc.98.044321_references_DOI_NSeEndFdYBMLwcoCjFmWypsF6Dn"},{"@type":"CROSSREF","@value":"10.1140/epja/i2017-12367-5_references_DOI_NSeEndFdYBMLwcoCjFmWypsF6Dn"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptab126_references_DOI_NSeEndFdYBMLwcoCjFmWypsF6Dn"},{"@type":"CROSSREF","@value":"10.1103/revmodphys.85.693_references_DOI_NSeEndFdYBMLwcoCjFmWypsF6Dn"},{"@type":"CROSSREF","@value":"10.1007/s11467-018-0846-3_references_DOI_NSeEndFdYBMLwcoCjFmWypsF6Dn"},{"@type":"CROSSREF","@value":"10.1103/physrevc.98.014308_references_DOI_NSeEndFdYBMLwcoCjFmWypsF6Dn"},{"@type":"CROSSREF","@value":"10.1103/physrevc.98.044303_references_DOI_NSeEndFdYBMLwcoCjFmWypsF6Dn"},{"@type":"CROSSREF","@value":"10.1103/physrevc.103.024318_references_DOI_NSeEndFdYBMLwcoCjFmWypsF6Dn"}]}