FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2104076719> ?p ?o ?g. }

• W2104076719 endingPage "14" @default.
• W2104076719 startingPage "3" @default.
• W2104076719 abstract "We discuss dynamically the fusion–fission mechanism in the superheavy mass region. By analyzing the mass distribution of fission fragments, we distinguish between the fusion–fission process and the quasi-fission process. We investigate these two processes using the fluctuation–dissipation model. The three-dimensional Langevin equation is employed. We classify the dynamical process by analyzing the trajectory in the nuclear deformation space. In the superheavy mass region, we found that 90–99% of mass symmetric fission events come from the quasi-fission process, in which the system hardly reaches the spherical region. The fusion cross section is also estimated precisely." @default.
• W2104076719 created "2016-06-24" @default.
• W2104076719 creator A5051618851 @default.
• W2104076719 creator A5079037899 @default.
• W2104076719 date "2004-11-01" @default.
• W2104076719 modified "2023-09-30" @default.
• W2104076719 title "Dynamical calculation for fusion–fission probability in superheavy mass region, where mass symmetric fission events originate" @default.
• W2104076719 cites W153451775 @default.
• W2104076719 cites W1558183314 @default.
• W2104076719 cites W1619585869 @default.
• W2104076719 cites W1967197855 @default.
• W2104076719 cites W1971299349 @default.
• W2104076719 cites W1976222174 @default.
• W2104076719 cites W1988269009 @default.
• W2104076719 cites W1988444145 @default.
• W2104076719 cites W1994355881 @default.
• W2104076719 cites W2001475423 @default.
• W2104076719 cites W2002426297 @default.
• W2104076719 cites W2009714980 @default.
• W2104076719 cites W2011797910 @default.
• W2104076719 cites W2012012474 @default.
• W2104076719 cites W2022688138 @default.
• W2104076719 cites W2022795578 @default.
• W2104076719 cites W2023095574 @default.
• W2104076719 cites W2039070775 @default.
• W2104076719 cites W2040796111 @default.
• W2104076719 cites W2042198619 @default.
• W2104076719 cites W2049602977 @default.
• W2104076719 cites W2052592567 @default.
• W2104076719 cites W2054577557 @default.
• W2104076719 cites W2057564392 @default.
• W2104076719 cites W2060227816 @default.
• W2104076719 cites W2069219303 @default.
• W2104076719 cites W2077573271 @default.
• W2104076719 cites W2080272910 @default.
• W2104076719 cites W2093859556 @default.
• W2104076719 cites W2094175853 @default.
• W2104076719 cites W2094866626 @default.
• W2104076719 cites W2099088053 @default.
• W2104076719 cites W2139735186 @default.
• W2104076719 cites W2141790717 @default.
• W2104076719 cites W2156317929 @default.
• W2104076719 cites W2169605949 @default.
• W2104076719 cites W2297270199 @default.
• W2104076719 cites W2492674117 @default.
• W2104076719 cites W2988248053 @default.
• W2104076719 cites W4253059346 @default.
• W2104076719 doi "https://doi.org/10.1016/j.nuclphysa.2004.08.009" @default.
• W2104076719 hasPublicationYear "2004" @default.
• W2104076719 type Work @default.
• W2104076719 sameAs 2104076719 @default.
• W2104076719 citedByCount "72" @default.
• W2104076719 countsByYear W21040767192012 @default.
• W2104076719 countsByYear W21040767192013 @default.
• W2104076719 countsByYear W21040767192014 @default.
• W2104076719 countsByYear W21040767192015 @default.
• W2104076719 countsByYear W21040767192016 @default.
• W2104076719 countsByYear W21040767192017 @default.
• W2104076719 countsByYear W21040767192018 @default.
• W2104076719 countsByYear W21040767192019 @default.
• W2104076719 countsByYear W21040767192020 @default.
• W2104076719 countsByYear W21040767192021 @default.
• W2104076719 countsByYear W21040767192022 @default.
• W2104076719 countsByYear W21040767192023 @default.
• W2104076719 crossrefType "journal-article" @default.
• W2104076719 hasAuthorship W2104076719A5051618851 @default.
• W2104076719 hasAuthorship W2104076719A5079037899 @default.
• W2104076719 hasConcept C121332964 @default.
• W2104076719 hasConcept C12294094 @default.
• W2104076719 hasConcept C134222618 @default.
• W2104076719 hasConcept C152568617 @default.
• W2104076719 hasConcept C15522600 @default.
• W2104076719 hasConcept C185544564 @default.
• W2104076719 hasConcept C36091686 @default.
• W2104076719 hasConcept C62520636 @default.
• W2104076719 hasConcept C98444146 @default.
• W2104076719 hasConceptScore W2104076719C121332964 @default.
• W2104076719 hasConceptScore W2104076719C12294094 @default.
• W2104076719 hasConceptScore W2104076719C134222618 @default.
• W2104076719 hasConceptScore W2104076719C152568617 @default.
• W2104076719 hasConceptScore W2104076719C15522600 @default.
• W2104076719 hasConceptScore W2104076719C185544564 @default.
• W2104076719 hasConceptScore W2104076719C36091686 @default.
• W2104076719 hasConceptScore W2104076719C62520636 @default.
• W2104076719 hasConceptScore W2104076719C98444146 @default.
• W2104076719 hasLocation W21040767191 @default.
• W2104076719 hasOpenAccess W2104076719 @default.
• W2104076719 hasPrimaryLocation W21040767191 @default.
• W2104076719 hasRelatedWork W109353549 @default.
• W2104076719 hasRelatedWork W1977860546 @default.
• W2104076719 hasRelatedWork W2008614562 @default.
• W2104076719 hasRelatedWork W2014090056 @default.
• W2104076719 hasRelatedWork W2014381587 @default.
• W2104076719 hasRelatedWork W2039324293 @default.
• W2104076719 hasRelatedWork W2078752668 @default.
• W2104076719 hasRelatedWork W2082009486 @default.
• W2104076719 hasRelatedWork W3196253290 @default.
• W2104076719 hasRelatedWork W4380591300 @default.

• next