{"@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/1360004236127409408.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1140/epja/i2016-16373-9"}},{"identifier":{"@type":"URI","@value":"http://link.springer.com/content/pdf/10.1140/epja/i2016-16373-9.pdf"}},{"identifier":{"@type":"URI","@value":"http://link.springer.com/article/10.1140/epja/i2016-16373-9/fulltext.html"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1612.09432"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"Antisymmetrized molecular dynamics studies for exotic clustering phenomena in neutron-rich nuclei"}],"description":[{"notation":[{"@value":"We present a review of recent works on clustering phenomena in unstable nuclei studied by antisymmetrized molecular dynamics (AMD). The AMD studies in these decades have uncovered novel types of clustering phenomena brought about by the excess neutrons. Among them, this review focuses on the molecule-like structure of unstable nuclei. One of the earliest discussions on the clustering in unstable nuclei was made for neutron-rich Be and B isotopes. AMD calculations predicted that the ground state clustering is enhanced or reduced depending on the number of excess neutrons. Today, the experiments are confirming this prediction as the change of the proton radii. Behind this enhancement and reduction of the clustering, there are underlying shell effects called molecular- and atomic-orbits. These orbits form covalent and ionic bonding of the clusters analogous to the atomic molecules. It was found that this \"molecular-orbit picture\" reasonably explains the low-lying spectra of Be isotopes. The molecular-orbit picture is extended to other systems having parity asymmetric cluster cores and to the three cluster systems. O and Ne isotopes are the candidates of the former, while the $3��$ linear chains in C isotopes are the latter. For both subjects, many intensive studies are now in progress. We also pay a special attention to the observables which are the fingerprint of the clustering. In particular, we focus on the monopole and dipole transitions which are recently regarded as good probe for the clustering. We discuss how they have and will reveal the exotic clustering."}]},{"notation":[{"@value":"96 pages, 44 figures"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380004231464776967","@type":"Researcher","foaf:name":[{"@value":"M. Kimura"}]},{"@id":"https://cir.nii.ac.jp/crid/1380004236127406990","@type":"Researcher","foaf:name":[{"@value":"T. Suhara"}]},{"@id":"https://cir.nii.ac.jp/crid/1380004236127406849","@type":"Researcher","foaf:name":[{"@value":"Y. Kanada-En’yo"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"14346001"},{"@type":"EISSN","@value":"1434601X"}],"prism:publicationName":[{"@value":"The European Physical Journal A"}],"dc:publisher":[{"@value":"Springer Science and Business Media LLC"}],"prism:publicationDate":"2016-12","prism:volume":"52","prism:number":"12","prism:startingPage":"373"},"reviewed":"false","dc:rights":["http://www.springer.com/tdm"],"url":[{"@id":"http://link.springer.com/content/pdf/10.1140/epja/i2016-16373-9.pdf"},{"@id":"http://link.springer.com/article/10.1140/epja/i2016-16373-9/fulltext.html"}],"createdAt":"2016-12-29","modifiedAt":"2022-07-20","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=Nuclear%20Theory%20(nucl-th)","dc:title":"Nuclear Theory (nucl-th)"},{"@id":"https://cir.nii.ac.jp/all?q=Nuclear%20Theory","dc:title":"Nuclear Theory"},{"@id":"https://cir.nii.ac.jp/all?q=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"}],"project":[{"@id":"https://cir.nii.ac.jp/crid/1040000781911090944","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"16K05339"},{"@type":"JGN","@value":"JP16K05339"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-16K05339/"}],"notation":[{"@language":"ja","@value":"単極、双極遷移をプローブとするクラスター共鳴の探査と炭素燃焼過程への応用"},{"@language":"en","@value":"Study of cluster resonances probed by monopole and dipole transitions, and its application to Carbon burning process"}]},{"@id":"https://cir.nii.ac.jp/crid/1040000782189462528","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"24105008"},{"@type":"JGN","@value":"JP24105008"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PLANNED-24105008/"}],"notation":[{"@language":"ja","@value":"中性子星と核物質の理論研究"},{"@language":"en","@value":"Theoretical Study of Neutron Stars and Nuclear Matter"}]},{"@id":"https://cir.nii.ac.jp/crid/1040000782297484928","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"26400270"},{"@type":"JGN","@value":"JP26400270"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-26400270/"}],"notation":[{"@language":"ja","@value":"微視的効果を取り入れた原子核散乱の記述と原子核反応への応用"},{"@language":"en","@value":"Microscopic description of nuclear scattering and application  to nuclear reactions"}]},{"@id":"https://cir.nii.ac.jp/crid/1040282256839224320","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"15K17662"},{"@type":"JGN","@value":"JP15K17662"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-15K17662/"}],"notation":[{"@language":"ja","@value":"余剰中性子によるクラスター構造安定化機構の解明"},{"@language":"en","@value":"Investigation of the stabilization mechanism of cluster structures owing to excess 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xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mrow/><mml:mn>10</mml:mn></mml:msup></mml:math>Be"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235000507904","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Mapping the deformation in the “island of inversion”: Inelastic scattering of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi>Ne</mml:mi><mml:mprescripts/><mml:none/><mml:mn>30</mml:mn></mml:mmultiscripts></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi>Mg</mml:mi><mml:mprescripts/><mml:none/><mml:mn>36</mml:mn></mml:mmultiscripts></mml:math>at intermediate energies"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235000537472","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Deformation effects on isoscalar giant 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radii: properties of the radius surface R(N,Z)"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418519453237632","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Molecular dynamics for fermions"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418519538521088","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Evidence for a molecular rotational band in the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>14</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant=\"normal\">C</mml:mi><mml:mo>+</mml:mo><mml:mi>α</mml:mi></mml:math>decay of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>18</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant=\"normal\">O</mml:mi></mml:math>and the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>α</mml:mi></mml:math>decay of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>22</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant=\"normal\">Ne</mml:mi></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418519633088000","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Resonances in<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:mrow><mml:mn>14</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>observed in the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">He</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:mmultiscripts><mml:mo>(</mml:mo><mml:mrow><mml:msup><mml:mrow/><mml:mn>10</mml:mn></mml:msup><mml:mi>Be</mml:mi><mml:mo>,</mml:mo><mml:mi>α</mml:mi></mml:mrow><mml:mo>)</mml:mo><mml:mmultiscripts><mml:mi mathvariant=\"normal\">Be</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>10</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>reaction"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418519852317824","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Weak coupling model of particles and holes in the sd shell nuclei"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520024323840","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Coexistence of Cluster States and Mean-Field-Type States"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520043506048","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Spectroscopy of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">O</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>18</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>: Radiative capture,<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant=\"italic\">α</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>14</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>,γ<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>18</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>O"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520464268800","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Further Improvement of the Upper Limit on the Direct<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mn>3</mml:mn><mml:mi>α</mml:mi></mml:mrow></mml:math>Decay from the Hoyle State in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">C</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520759799168","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Reduced widths in O16 and gamma transition probabilities in F19"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520782952960","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Microscopic description of the α<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mo>+</mml:mo></mml:mrow><mml:mrow><mml:mn>16</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>O system in a multicluster model"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520783987712","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Antisymmetrized Molecular Dynamics: a new insight into the structure of nuclei"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520839108096","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Cluster breakup of<sup>18</sup>O and<sup>22</sup>Ne"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520885345280","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"New experimental investigation of the structure of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi>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\">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>16</mml:mn></mml:mmultiscripts></mml:math>by means of intermediate-energy sequential breakup"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520899070976","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"High lying<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>E</mml:mi><mml:mn>0</mml:mn><mml:mn/></mml:math>strength in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant=\"normal\">C</mml:mi></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418521175275136","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Spectroscopy of 13Be"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418521313792640","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Proton single-particle states in the neutron-rich 23F nucleus"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418521366903936","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Quadrupole collectivity of 28Ne and the boundary of the island of inversion"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699993390474624","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Rotational Bands in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">Ne</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>22</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>Excited by the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">O</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>18</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">Li</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>7</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">Ne</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>22</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>Reaction"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699993422841600","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Spectroscopy of 12Be and 13Be using a 12Be radioactive beam"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699993540352640","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Beta decay of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">Na</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>2</mml:mn><mml:mn>7</mml:mn><mml:mo>−</mml:mo><mml:mn>3</mml:mn><mml:mn>2</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>and their descendants"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994221019136","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Two-center molecular states in9B,9Be,10Be, and10B"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994280625152","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Microscopic study of α clustering in the 9,10,11Be isotopes"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995212048256","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Covalently bound molecular states in beryllium and carbon isotopes"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995372050432","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Application of the generalized two-center cluster model to 10Be"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995590701056","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Triple configuration coexistence in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">S</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>44</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995818372480","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Decay properties of exotic<i>N</i>≃28 S and Cl nuclei and the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">Ca</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>48</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mo>/</mml:mo></mml:mrow><mml:mrow><mml:mn>46</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>Ca abundance ratio"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699996154134912","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Systematic investigation of the drip-line nuclei 11Li and 14Be and their unbound subsystems 10Li and 13Be"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699996461159936","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Total nuclear photon absorption cross sections for some light elements"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468540067200","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Variation after Angular Momentum Projection for the Study of Excited States Based on Antisymmetrized Molecular Dynamics"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468704127104","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Sequential decay reactions induced by a 18 MeV 6He beam on 6Li and 7Li"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468796828800","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Extreme $ \\alpha$ -clustering in the 18O nucleus"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468844179456","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Nuclear magic numbers: New features far from stability"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981469191033216","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"TRANSITION PROBABILITY FROM THE GROUND TO THE FIRST-EXCITED 2+ STATE OF EVEN–EVEN NUCLIDES"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981469417037312","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"First observation of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>α</mml:mi></mml:mrow></mml:math>-cluster states in the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mn>14</mml:mn></mml:mrow></mml:msup><mml:mi mathvariant=\"normal\">O</mml:mi><mml:mi> </mml:mi><mml:mo>+</mml:mo><mml:mi> </mml:mi><mml:msup><mml:mi/><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msup><mml:mi mathvariant=\"normal\">He</mml:mi></mml:mrow></mml:math>interaction"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981469541953920","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Vanishing of the shell gap in N = 20 neutron-rich nuclei"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981469556122880","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Cluster structure in stable and unstable nuclei"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470325445504","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>p</mml:mi><mml:mtext mathvariant=\"normal\">−</mml:mtext><mml:mi>s</mml:mi><mml:mi>d</mml:mi></mml:math>Shell Gap Reduction in Neutron-Rich Systems and Cross-Shell Excitations in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">O</mml:mi><mml:mprescripts/><mml:none/><mml:mn>20</mml:mn></mml:mmultiscripts></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470360807296","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Coexistence of Single-Particle, Collective-Quadrupole, and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>α</mml:mi></mml:math>+<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">C</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>14</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>Molecular-Dipole Degrees of Freedom in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">O</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>18</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470696443264","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Energy levels of light nuclei, A = 20"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470702715392","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Proton pick-up from 19F, 20Ne and 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