Matches in SemOpenAlex for { <https://semopenalex.org/work/W2024052105> ?p ?o ?g. }
Showing items 1 to 74 of
74
with 100 items per page.
- W2024052105 abstract "Abstract Some arguments are presented in favor of an interpretation of the asymmetric fission, in which the light fission fragments are considered as being formed from the valence shells of the fissile nuclei. E.g., the peak-to-peak distance of the mass yield curve for neutron-induced fission is found to vary linearly with the number N p + N n of valence nucleons of the system undergoing fission. A detailed description of the asymmetric fission can be given, e.g. of 240Pu, which is based on binding energy calculations (energy release = 216.868 MeV) and energy relations holding in the valence shells. The neutron-proton interaction energy within the valence shells is proportional to the number N p × N n of n-p couples. Two methods are proposed for the calculation of E np . For 240 Pu, E np is about 63 MeV, i.e. the interaction energy per n-p couple is 263.1 keV. Other interaction laws between valence nucleons are described: the n-2n and 2n-2n repulsion laws, and the p-2p and 2p-2p repulsion laws. In even-even nuclei, the energy binding all the valence proton pairs is p · gs 2p , where p is the number of proton pairs and σ 2p a mean “from core” separation energy per proton pair. Its value is independent of the number of pairs of nucleons of the other kind. For 240Pu, the energy binding any one of the six proton pairs to the core is only 5050 keV, and the energy binding any one of the ten neutron pairs to the core is as great as 8358 keV. This means that the protons are farther from the core than the neutrons. As the energy binding the protons to the core decreases rapidly with Z, and could be zero for Z = 108 , neutrons have to be seen as bridges binding to the core the protons of the valence shell in the heavy actinides. This situation, and the weakness of all the valence shell interaction energies, explain that a neutron can induce shell alterations permitting the onset of stronger nuclear forces and nuclear fission." @default.
- W2024052105 created "2016-06-24" @default.
- W2024052105 creator A5058534171 @default.
- W2024052105 creator A5084587156 @default.
- W2024052105 date "1989-07-01" @default.
- W2024052105 modified "2023-09-27" @default.
- W2024052105 title "New points of view on the nuclear properties of the fissile actinides" @default.
- W2024052105 cites W2047305573 @default.
- W2024052105 cites W2065179599 @default.
- W2024052105 cites W2083382400 @default.
- W2024052105 cites W2087857662 @default.
- W2024052105 cites W2596887009 @default.
- W2024052105 cites W3021045830 @default.
- W2024052105 doi "https://doi.org/10.1016/0022-3115(89)90178-5" @default.
- W2024052105 hasPublicationYear "1989" @default.
- W2024052105 type Work @default.
- W2024052105 sameAs 2024052105 @default.
- W2024052105 citedByCount "1" @default.
- W2024052105 crossrefType "journal-article" @default.
- W2024052105 hasAuthorship W2024052105A5058534171 @default.
- W2024052105 hasAuthorship W2024052105A5084587156 @default.
- W2024052105 hasConcept C121332964 @default.
- W2024052105 hasConcept C12294094 @default.
- W2024052105 hasConcept C152568617 @default.
- W2024052105 hasConcept C168900304 @default.
- W2024052105 hasConcept C172695262 @default.
- W2024052105 hasConcept C184779094 @default.
- W2024052105 hasConcept C185544564 @default.
- W2024052105 hasConcept C185592680 @default.
- W2024052105 hasConcept C54516573 @default.
- W2024052105 hasConcept C62520636 @default.
- W2024052105 hasConcept C75812238 @default.
- W2024052105 hasConcept C78310665 @default.
- W2024052105 hasConcept C93282013 @default.
- W2024052105 hasConceptScore W2024052105C121332964 @default.
- W2024052105 hasConceptScore W2024052105C12294094 @default.
- W2024052105 hasConceptScore W2024052105C152568617 @default.
- W2024052105 hasConceptScore W2024052105C168900304 @default.
- W2024052105 hasConceptScore W2024052105C172695262 @default.
- W2024052105 hasConceptScore W2024052105C184779094 @default.
- W2024052105 hasConceptScore W2024052105C185544564 @default.
- W2024052105 hasConceptScore W2024052105C185592680 @default.
- W2024052105 hasConceptScore W2024052105C54516573 @default.
- W2024052105 hasConceptScore W2024052105C62520636 @default.
- W2024052105 hasConceptScore W2024052105C75812238 @default.
- W2024052105 hasConceptScore W2024052105C78310665 @default.
- W2024052105 hasConceptScore W2024052105C93282013 @default.
- W2024052105 hasLocation W20240521051 @default.
- W2024052105 hasOpenAccess W2024052105 @default.
- W2024052105 hasPrimaryLocation W20240521051 @default.
- W2024052105 hasRelatedWork W121101190 @default.
- W2024052105 hasRelatedWork W135429434 @default.
- W2024052105 hasRelatedWork W1643436170 @default.
- W2024052105 hasRelatedWork W1980027475 @default.
- W2024052105 hasRelatedWork W1986539436 @default.
- W2024052105 hasRelatedWork W1988662550 @default.
- W2024052105 hasRelatedWork W1999506010 @default.
- W2024052105 hasRelatedWork W2004980357 @default.
- W2024052105 hasRelatedWork W2019337564 @default.
- W2024052105 hasRelatedWork W2052890871 @default.
- W2024052105 hasRelatedWork W2056961460 @default.
- W2024052105 hasRelatedWork W2080412864 @default.
- W2024052105 hasRelatedWork W2164269084 @default.
- W2024052105 hasRelatedWork W2271482291 @default.
- W2024052105 hasRelatedWork W2273757124 @default.
- W2024052105 hasRelatedWork W2312550344 @default.
- W2024052105 hasRelatedWork W2810039896 @default.
- W2024052105 hasRelatedWork W3042410784 @default.
- W2024052105 hasRelatedWork W2184677541 @default.
- W2024052105 hasRelatedWork W2469483937 @default.
- W2024052105 isParatext "false" @default.
- W2024052105 isRetracted "false" @default.
- W2024052105 magId "2024052105" @default.
- W2024052105 workType "article" @default.