{"@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/1361699994969627520.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevc.59.817"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevC.59.817"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevC.59.817/fulltext"}},{"identifier":{"@type":"HANDLE","@value":"2013/ULB-DIPOT:oai:dipot.ulb.ac.be:2013/47558"}}],"dc:title":[{"@value":"Low-energy<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>α</mml:mi><mml:mrow><mml:msup><mml:mrow><mml:mo>+</mml:mo></mml:mrow><mml:mrow><mml:mn>6</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant=\"normal\">He</mml:mi></mml:math>elastic scattering with the resonating-group method"}],"description":[{"notation":[{"@value":"The $\\ensuremath{\\alpha}{+}^{6}\\mathrm{He}$ elastic scattering is investigated within a microscopic multicluster model, involving a realistic description of the ${}^{6}\\mathrm{He}$ halo nucleus. Phase shifts and elastic-scattering cross sections are calculated up to ${E}_{\\mathrm{c}.\\mathrm{m}.}=15 \\mathrm{MeV}$ with two variants of the resonating-group method. The model gives rise to ${1}^{\\ensuremath{-}}$ and ${3}^{\\ensuremath{-}}$ molecular states near ${E}_{\\mathrm{c}.\\mathrm{m}.}=0.5 \\mathrm{MeV}$ and ${E}_{\\mathrm{c}.\\mathrm{m}.}=3.7 \\mathrm{MeV},$ respectively. We suggest that the broad ${3}^{\\ensuremath{-}}$ resonance should be observable by comparing elastic cross sections at different energies. We also evaluate the order of magnitude of the ${}^{6}\\mathrm{He}$ breakup cross section."}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381699994969627521","@type":"Researcher","foaf:name":[{"@value":"K. Fujimura"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994969627524","@type":"Researcher","foaf:name":[{"@value":"D. Baye"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994969627520","@type":"Researcher","foaf:name":[{"@value":"P. Descouvemont"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994969627522","@type":"Researcher","foaf:name":[{"@value":"Y. Suzuki"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994969627523","@type":"Researcher","foaf:name":[{"@value":"K. Varga"}]}],"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":"1999-02-01","prism:volume":"59","prism:number":"2","prism:startingPage":"817","prism:endingPage":"825"},"reviewed":"false","dc:rights":["http://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"http://link.aps.org/article/10.1103/PhysRevC.59.817"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevC.59.817/fulltext"}],"createdAt":"2002-07-26","modifiedAt":"2017-06-15","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=Physique","dc:title":"Physique"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050845760771200128","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Monopole transitions to cluster states in [10]Be and [9]Li"},{"@value":"Monopole transitions to cluster states in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">Be</mml:mi><mml:mprescripts/><mml:none/><mml:mn>10</mml:mn></mml:mmultiscripts></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">Li</mml:mi><mml:mprescripts/><mml:none/><mml:mn>9</mml:mn></mml:mmultiscripts></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360283692797196160","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mrow/><mml:mn>6</mml:mn></mml:msup></mml:math>He-triton cluster states in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mrow/><mml:mn>9</mml:mn></mml:msup></mml:math>Li"}]},{"@id":"https://cir.nii.ac.jp/crid/2050307417125183616","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Variation after K-projection in antisymmetrized molecular dynamics for low-energy dipole excitations in 10Be and 16O"}]},{"@id":"https://cir.nii.ac.jp/crid/2050870367067396608","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Approximation of reduced width amplitude and application to cluster decay width"}]},{"@id":"https://cir.nii.ac.jp/crid/2051433317031873920","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"A stochastic microscopic approach to the 10Be and 11Be nuclei"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1103/physrevc.59.817"},{"@type":"OPENAIRE","@value":"doi_dedup___::d2f7aecee63c4d8d7e07ba93f1f1ff31"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptu095_references_DOI_WOJQatCSZkOwkp7HcN06tYwJR5x"},{"@type":"CROSSREF","@value":"10.1103/physrevc.85.024303_references_DOI_WOJQatCSZkOwkp7HcN06tYwJR5x"},{"@type":"CROSSREF","@value":"10.1103/physrevc.94.024326_references_DOI_WOJQatCSZkOwkp7HcN06tYwJR5x"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptaa092_references_DOI_WOJQatCSZkOwkp7HcN06tYwJR5x"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptz169_references_DOI_WOJQatCSZkOwkp7HcN06tYwJR5x"}]}