FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W4386033091> ?p ?o ?g. }

• W4386033091 abstract "The yield distributions of neutron-induced fission of actinides were calculated and evaluated by using the improved scission-point model with considering octupole deformation of fragments. We studied the influence of the octupole deformation on the asymmetric yields of actinides fission. The more probable scission configuration is the pear-shaped heavy fragments rather than more spherical shape. We used the improved scission model to calculate the peak of charge and neutron distributions and compared results with the experimental data. The results confirm that the main asymmetric fission mode of the heavy actinides fission is indeed characterized by ``${mathrm{Z}}_{mathrm{H}}ensuremath{approx}54$.'' The protons configuration of heavy fragment plays a dominant role in asymmetric fission of actinides." @default.
• W4386033091 created "2023-08-22" @default.
• W4386033091 creator A5017532188 @default.
• W4386033091 creator A5019610756 @default.
• W4386033091 creator A5025541319 @default.
• W4386033091 creator A5027816381 @default.
• W4386033091 creator A5052807800 @default.
• W4386033091 creator A5055447339 @default.
• W4386033091 creator A5055847877 @default.
• W4386033091 creator A5056334408 @default.
• W4386033091 creator A5057351016 @default.
• W4386033091 creator A5068367513 @default.
• W4386033091 creator A5073741830 @default.
• W4386033091 date "2023-08-21" @default.
• W4386033091 modified "2023-10-17" @default.
• W4386033091 title "Effect of octupole deformation of fragments on mass-asymmetric yields of fission of actinide nuclei" @default.
• W4386033091 cites W1968514256 @default.
• W4386033091 cites W1974157972 @default.
• W4386033091 cites W1991715522 @default.
• W4386033091 cites W1997962918 @default.
• W4386033091 cites W1999425086 @default.
• W4386033091 cites W2005468328 @default.
• W4386033091 cites W2026465169 @default.
• W4386033091 cites W2077343341 @default.
• W4386033091 cites W2079505573 @default.
• W4386033091 cites W2086065566 @default.
• W4386033091 cites W2159777974 @default.
• W4386033091 cites W2162693255 @default.
• W4386033091 cites W2169910634 @default.
• W4386033091 cites W2280630311 @default.
• W4386033091 cites W2346357926 @default.
• W4386033091 cites W2506265244 @default.
• W4386033091 cites W2563773455 @default.
• W4386033091 cites W2598962353 @default.
• W4386033091 cites W2761008975 @default.
• W4386033091 cites W2791114124 @default.
• W4386033091 cites W2792161924 @default.
• W4386033091 cites W2905524202 @default.
• W4386033091 cites W2924088880 @default.
• W4386033091 cites W2950065585 @default.
• W4386033091 cites W2973394994 @default.
• W4386033091 cites W2976866703 @default.
• W4386033091 cites W3012194603 @default.
• W4386033091 cites W3033400662 @default.
• W4386033091 cites W3180217861 @default.
• W4386033091 cites W3197639327 @default.
• W4386033091 cites W4293834848 @default.
• W4386033091 doi "https://doi.org/10.1103/physrevc.108.024608" @default.
• W4386033091 hasPublicationYear "2023" @default.
• W4386033091 type Work @default.
• W4386033091 citedByCount "0" @default.
• W4386033091 crossrefType "journal-article" @default.
• W4386033091 hasAuthorship W4386033091A5017532188 @default.
• W4386033091 hasAuthorship W4386033091A5019610756 @default.
• W4386033091 hasAuthorship W4386033091A5025541319 @default.
• W4386033091 hasAuthorship W4386033091A5027816381 @default.
• W4386033091 hasAuthorship W4386033091A5052807800 @default.
• W4386033091 hasAuthorship W4386033091A5055447339 @default.
• W4386033091 hasAuthorship W4386033091A5055847877 @default.
• W4386033091 hasAuthorship W4386033091A5056334408 @default.
• W4386033091 hasAuthorship W4386033091A5057351016 @default.
• W4386033091 hasAuthorship W4386033091A5068367513 @default.
• W4386033091 hasAuthorship W4386033091A5073741830 @default.
• W4386033091 hasConcept C103522932 @default.
• W4386033091 hasConcept C121332964 @default.
• W4386033091 hasConcept C12294094 @default.
• W4386033091 hasConcept C134121241 @default.
• W4386033091 hasConcept C135788738 @default.
• W4386033091 hasConcept C152568617 @default.
• W4386033091 hasConcept C153336213 @default.
• W4386033091 hasConcept C184779094 @default.
• W4386033091 hasConcept C185544564 @default.
• W4386033091 hasConcept C43997528 @default.
• W4386033091 hasConcept C76258055 @default.
• W4386033091 hasConcept C77016745 @default.
• W4386033091 hasConcept C97355855 @default.
• W4386033091 hasConceptScore W4386033091C103522932 @default.
• W4386033091 hasConceptScore W4386033091C121332964 @default.
• W4386033091 hasConceptScore W4386033091C12294094 @default.
• W4386033091 hasConceptScore W4386033091C134121241 @default.
• W4386033091 hasConceptScore W4386033091C135788738 @default.
• W4386033091 hasConceptScore W4386033091C152568617 @default.
• W4386033091 hasConceptScore W4386033091C153336213 @default.
• W4386033091 hasConceptScore W4386033091C184779094 @default.
• W4386033091 hasConceptScore W4386033091C185544564 @default.
• W4386033091 hasConceptScore W4386033091C43997528 @default.
• W4386033091 hasConceptScore W4386033091C76258055 @default.
• W4386033091 hasConceptScore W4386033091C77016745 @default.
• W4386033091 hasConceptScore W4386033091C97355855 @default.
• W4386033091 hasFunder F4320321001 @default.
• W4386033091 hasFunder F4320336808 @default.
• W4386033091 hasIssue "2" @default.
• W4386033091 hasLocation W43860330911 @default.
• W4386033091 hasOpenAccess W4386033091 @default.
• W4386033091 hasPrimaryLocation W43860330911 @default.
• W4386033091 hasRelatedWork W1983390678 @default.
• W4386033091 hasRelatedWork W1987391621 @default.
• W4386033091 hasRelatedWork W2010830995 @default.
• W4386033091 hasRelatedWork W2030436833 @default.
• W4386033091 hasRelatedWork W2077281778 @default.

• next