Matches in SemOpenAlex for { <https://semopenalex.org/work/W2121661552> ?p ?o ?g. }
Showing items 1 to 93 of
93
with 100 items per page.
- W2121661552 endingPage "012011" @default.
- W2121661552 startingPage "012011" @default.
- W2121661552 abstract "A systematic investigation of the properties of hot nuclei may be studied by detecting the evaporated particles. These emissions reflect the behavior of the nucleus at various stages of the deexcitation cascade. When the nucleus is formed by the collision of a heavy nucleus with a light particle, the statistical model has done a good job of predicting the distribution of evaporated particles when reasonable choices were made for the level densities and yrast lines. Comparison to more specific measurements could, of course, provide a more severe test of the model and enable one to identify the deviations from the statistical model as the signature of other effects not included in the model. Some papers have claimed that experimental evaporation spectra from heavy-ion fusion reactions at higher excitation energies and angular momenta are no longer consistent with the predictions of the standard statistical model. In order to confirm this prediction we have employed two systems, a mass-symmetric (31P+45Sc) and a mass-asymmetric channel (12C+64Zn), leading to the same compound nucleus 76Kr* at the excitation energy of 75 MeV. Neutron energy spectra of the asymmetric system (12C+64Zn) at different angles are well described by the statistical model predictions using the normal value of the level density parameter a = A/8 MeV−1. However, in the case of the symmetric system (31P+45Sc), the statistical model interpretation of the data requires the change in the value of a = A/10 MeV−1. The delayed evolution of the compound system in case of the symmetric 31P+45Sc system may lead to the formation of a temperature equilibrated dinuclear complex, which may be responsible for the neutron emission at higher temperature, while the protons and alpha particles are evaporated after neutron emission when the system is sufficiently cooled down and the higher g-values do not contribute in the formation of the compound nucleus for the symmetric entrance channel in case of charged particle emission." @default.
- W2121661552 created "2016-06-24" @default.
- W2121661552 creator A5029171581 @default.
- W2121661552 date "2014-05-14" @default.
- W2121661552 modified "2023-09-25" @default.
- W2121661552 title "Study of angular momentum variation due to entrance channel effect in heavy ion fusion reactions" @default.
- W2121661552 cites W1608980625 @default.
- W2121661552 cites W1971389376 @default.
- W2121661552 cites W1988600737 @default.
- W2121661552 cites W1993016285 @default.
- W2121661552 cites W2001381752 @default.
- W2121661552 cites W2012012474 @default.
- W2121661552 cites W2018287321 @default.
- W2121661552 cites W2019412659 @default.
- W2121661552 cites W2019527512 @default.
- W2121661552 cites W2026276863 @default.
- W2121661552 cites W2034072535 @default.
- W2121661552 cites W2044223040 @default.
- W2121661552 cites W2044849857 @default.
- W2121661552 cites W2046638832 @default.
- W2121661552 cites W2050240992 @default.
- W2121661552 cites W2050714365 @default.
- W2121661552 cites W2064519611 @default.
- W2121661552 cites W2066296291 @default.
- W2121661552 cites W2071478636 @default.
- W2121661552 cites W2078251146 @default.
- W2121661552 cites W2078887214 @default.
- W2121661552 cites W2092199053 @default.
- W2121661552 cites W2093258580 @default.
- W2121661552 cites W2134042797 @default.
- W2121661552 cites W2511744552 @default.
- W2121661552 cites W285180181 @default.
- W2121661552 doi "https://doi.org/10.1088/1742-6596/515/1/012011" @default.
- W2121661552 hasPublicationYear "2014" @default.
- W2121661552 type Work @default.
- W2121661552 sameAs 2121661552 @default.
- W2121661552 citedByCount "1" @default.
- W2121661552 countsByYear W21216615522018 @default.
- W2121661552 crossrefType "journal-article" @default.
- W2121661552 hasAuthorship W2121661552A5029171581 @default.
- W2121661552 hasBestOaLocation W21216615521 @default.
- W2121661552 hasConcept C121332964 @default.
- W2121661552 hasConcept C127162648 @default.
- W2121661552 hasConcept C127413603 @default.
- W2121661552 hasConcept C1276947 @default.
- W2121661552 hasConcept C138885662 @default.
- W2121661552 hasConcept C145148216 @default.
- W2121661552 hasConcept C155675718 @default.
- W2121661552 hasConcept C158525013 @default.
- W2121661552 hasConcept C184779094 @default.
- W2121661552 hasConcept C185544564 @default.
- W2121661552 hasConcept C2778334786 @default.
- W2121661552 hasConcept C2988362075 @default.
- W2121661552 hasConcept C41895202 @default.
- W2121661552 hasConcept C62520636 @default.
- W2121661552 hasConcept C74650414 @default.
- W2121661552 hasConcept C76155785 @default.
- W2121661552 hasConceptScore W2121661552C121332964 @default.
- W2121661552 hasConceptScore W2121661552C127162648 @default.
- W2121661552 hasConceptScore W2121661552C127413603 @default.
- W2121661552 hasConceptScore W2121661552C1276947 @default.
- W2121661552 hasConceptScore W2121661552C138885662 @default.
- W2121661552 hasConceptScore W2121661552C145148216 @default.
- W2121661552 hasConceptScore W2121661552C155675718 @default.
- W2121661552 hasConceptScore W2121661552C158525013 @default.
- W2121661552 hasConceptScore W2121661552C184779094 @default.
- W2121661552 hasConceptScore W2121661552C185544564 @default.
- W2121661552 hasConceptScore W2121661552C2778334786 @default.
- W2121661552 hasConceptScore W2121661552C2988362075 @default.
- W2121661552 hasConceptScore W2121661552C41895202 @default.
- W2121661552 hasConceptScore W2121661552C62520636 @default.
- W2121661552 hasConceptScore W2121661552C74650414 @default.
- W2121661552 hasConceptScore W2121661552C76155785 @default.
- W2121661552 hasLocation W21216615521 @default.
- W2121661552 hasOpenAccess W2121661552 @default.
- W2121661552 hasPrimaryLocation W21216615521 @default.
- W2121661552 hasRelatedWork W1995562506 @default.
- W2121661552 hasRelatedWork W2052151044 @default.
- W2121661552 hasRelatedWork W2065921106 @default.
- W2121661552 hasRelatedWork W2073518606 @default.
- W2121661552 hasRelatedWork W2329112109 @default.
- W2121661552 hasRelatedWork W2622726516 @default.
- W2121661552 hasRelatedWork W2943752412 @default.
- W2121661552 hasRelatedWork W4253469476 @default.
- W2121661552 hasRelatedWork W4253600708 @default.
- W2121661552 hasRelatedWork W4280623212 @default.
- W2121661552 hasVolume "515" @default.
- W2121661552 isParatext "false" @default.
- W2121661552 isRetracted "false" @default.
- W2121661552 magId "2121661552" @default.
- W2121661552 workType "article" @default.