FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W1536469417> ?p ?o ?g. }

• W1536469417 endingPage "17" @default.
• W1536469417 startingPage "8" @default.
• W1536469417 abstract "Isomeric states for 4 nucleons with isospin T=1 are here considered. A comparison is made of the lighter and heavier members of cross-conjugate pairs where one member is obtained from the other by replacing protons by neutron holes and neutrons by proton holes. Although in the single j-shell the spectra in the two cases should be identical, this is not the case experimentally. For the former, the ground states all have angular momentum J=2. This result is found in a single j-shell calculation when the interaction is obtained from the spectrum of two particles. In a single j-shell (f7/2, g9/2) the state with angular momentum (2j−1) is the ground state for the heavier member of the pair provided one uses as an interaction the spectrum of two holes. The ground state behaviour can also be explained by rotational models. A new observation is that both in single j and in experiment the J=2 state in the heavier member and the (2j−1) state in the lighter member are isomeric." @default.
• W1536469417 created "2016-06-24" @default.
• W1536469417 creator A5015239979 @default.
• W1536469417 creator A5043034284 @default.
• W1536469417 date "2012-09-01" @default.
• W1536469417 modified "2023-09-30" @default.
• W1536469417 title "Single j-shell studies of cross-conjugate nuclei and isomerism: () rule" @default.
• W1536469417 cites W1965558889 @default.
• W1536469417 cites W1986616937 @default.
• W1536469417 cites W1988184500 @default.
• W1536469417 cites W2000977505 @default.
• W1536469417 cites W2019008803 @default.
• W1536469417 cites W2024569867 @default.
• W1536469417 cites W2034834282 @default.
• W1536469417 cites W2037193722 @default.
• W1536469417 cites W2041870549 @default.
• W1536469417 cites W2049247583 @default.
• W1536469417 cites W2049983086 @default.
• W1536469417 cites W2056999100 @default.
• W1536469417 cites W2066615294 @default.
• W1536469417 cites W2067412744 @default.
• W1536469417 cites W2071152694 @default.
• W1536469417 cites W2076423369 @default.
• W1536469417 cites W2077563906 @default.
• W1536469417 cites W2077771641 @default.
• W1536469417 cites W2080051312 @default.
• W1536469417 cites W2085177067 @default.
• W1536469417 cites W2085553982 @default.
• W1536469417 cites W2095270951 @default.
• W1536469417 cites W2162823695 @default.
• W1536469417 cites W2260562274 @default.
• W1536469417 cites W2470894790 @default.
• W1536469417 cites W2592043625 @default.
• W1536469417 doi "https://doi.org/10.1016/j.nuclphysa.2012.06.003" @default.
• W1536469417 hasPublicationYear "2012" @default.
• W1536469417 type Work @default.
• W1536469417 sameAs 1536469417 @default.
• W1536469417 citedByCount "13" @default.
• W1536469417 countsByYear W15364694172012 @default.
• W1536469417 countsByYear W15364694172013 @default.
• W1536469417 countsByYear W15364694172014 @default.
• W1536469417 countsByYear W15364694172015 @default.
• W1536469417 countsByYear W15364694172016 @default.
• W1536469417 countsByYear W15364694172017 @default.
• W1536469417 countsByYear W15364694172022 @default.
• W1536469417 crossrefType "journal-article" @default.
• W1536469417 hasAuthorship W1536469417A5015239979 @default.
• W1536469417 hasAuthorship W1536469417A5043034284 @default.
• W1536469417 hasBestOaLocation W15364694172 @default.
• W1536469417 hasConcept C10138342 @default.
• W1536469417 hasConcept C109214941 @default.
• W1536469417 hasConcept C117137515 @default.
• W1536469417 hasConcept C121332964 @default.
• W1536469417 hasConcept C152568617 @default.
• W1536469417 hasConcept C155675718 @default.
• W1536469417 hasConcept C159985019 @default.
• W1536469417 hasConcept C162324750 @default.
• W1536469417 hasConcept C172695262 @default.
• W1536469417 hasConcept C184779094 @default.
• W1536469417 hasConcept C185544564 @default.
• W1536469417 hasConcept C190284468 @default.
• W1536469417 hasConcept C192562407 @default.
• W1536469417 hasConcept C2777227988 @default.
• W1536469417 hasConcept C2781052500 @default.
• W1536469417 hasConcept C4839761 @default.
• W1536469417 hasConcept C54516573 @default.
• W1536469417 hasConcept C60718061 @default.
• W1536469417 hasConcept C62520636 @default.
• W1536469417 hasConcept C69523127 @default.
• W1536469417 hasConcept C88407732 @default.
• W1536469417 hasConceptScore W1536469417C10138342 @default.
• W1536469417 hasConceptScore W1536469417C109214941 @default.
• W1536469417 hasConceptScore W1536469417C117137515 @default.
• W1536469417 hasConceptScore W1536469417C121332964 @default.
• W1536469417 hasConceptScore W1536469417C152568617 @default.
• W1536469417 hasConceptScore W1536469417C155675718 @default.
• W1536469417 hasConceptScore W1536469417C159985019 @default.
• W1536469417 hasConceptScore W1536469417C162324750 @default.
• W1536469417 hasConceptScore W1536469417C172695262 @default.
• W1536469417 hasConceptScore W1536469417C184779094 @default.
• W1536469417 hasConceptScore W1536469417C185544564 @default.
• W1536469417 hasConceptScore W1536469417C190284468 @default.
• W1536469417 hasConceptScore W1536469417C192562407 @default.
• W1536469417 hasConceptScore W1536469417C2777227988 @default.
• W1536469417 hasConceptScore W1536469417C2781052500 @default.
• W1536469417 hasConceptScore W1536469417C4839761 @default.
• W1536469417 hasConceptScore W1536469417C54516573 @default.
• W1536469417 hasConceptScore W1536469417C60718061 @default.
• W1536469417 hasConceptScore W1536469417C62520636 @default.
• W1536469417 hasConceptScore W1536469417C69523127 @default.
• W1536469417 hasConceptScore W1536469417C88407732 @default.
• W1536469417 hasLocation W15364694171 @default.
• W1536469417 hasLocation W15364694172 @default.
• W1536469417 hasOpenAccess W1536469417 @default.
• W1536469417 hasPrimaryLocation W15364694171 @default.
• W1536469417 hasRelatedWork W1971816029 @default.
• W1536469417 hasRelatedWork W2049885251 @default.
• W1536469417 hasRelatedWork W2062720050 @default.

• next