{"@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/1363388845176989696.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevc.57.2760"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevC.57.2760"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevC.57.2760/fulltext"}}],"dc:title":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>α</mml:mi></mml:math>-cluster structure of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>44</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant=\"normal\">Ti</mml:mi></mml:math>in core-excited<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>40</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant=\"normal\">Ca</mml:mi></mml:math>model"}],"description":[{"notation":[{"@value":"It is shown that all the rotational bands in ${}^{44}\\mathrm{Ti}$ at low and high excitation energies can be well explained in an $\\ensuremath{\\alpha}$-cluster model in which the $\\ensuremath{\\alpha}$-like excitation of the core, ${}^{40}\\mathrm{Ca}$, is incorporated by employing density-dependent M3Y (DDM3Y) double folding potentials."}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1383388845176989697","@type":"Researcher","foaf:name":[{"@value":"S. Ohkubo"}]},{"@id":"https://cir.nii.ac.jp/crid/1383388845176989698","@type":"Researcher","foaf:name":[{"@value":"Y. Hirabayashi"}]},{"@id":"https://cir.nii.ac.jp/crid/1383388845176989696","@type":"Researcher","foaf:name":[{"@value":"T. Sakuda"}]}],"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":"1998-05-01","prism:volume":"57","prism:number":"5","prism:startingPage":"2760","prism:endingPage":"2762"},"reviewed":"false","dc:rights":["http://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"http://link.aps.org/article/10.1103/PhysRevC.57.2760"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevC.57.2760/fulltext"}],"createdAt":"2002-07-26","modifiedAt":"2017-06-15","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/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/2050870367078609152","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Bose-Einstein condensation of dilute alpha clusters above the four-α threshold in 16O in the 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/physrevc.57.2760"},{"@type":"OPENAIRE","@value":"doi_dedup___::a807fa68eb68c7735540a446e9962953"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptaa117_references_DOI_1aSIDUcsjqZZgqgSDO9t833vyO1"},{"@type":"CROSSREF","@value":"10.1080/00223131.2020.1769765_references_DOI_1aSIDUcsjqZZgqgSDO9t833vyO1"},{"@type":"CROSSREF","@value":"10.1103/physrevc.93.034319_references_DOI_1aSIDUcsjqZZgqgSDO9t833vyO1"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptab126_references_DOI_1aSIDUcsjqZZgqgSDO9t833vyO1"}]}