FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2149756022> ?p ?o ?g. }

• W2149756022 endingPage "51" @default.
• W2149756022 startingPage "35" @default.
• W2149756022 abstract "The excitation of a nucleus bombarded by nucleons of a few hundreds of MeV is considered as the result of individual interactions of the incoming nucleon with the nucleons of the nucleus. A simple two-particle model, in which a bombarding particle excites a particle moving in a potential well, has been calculated in the first Born approximation. It is shown that the resulting angular distributions have a strong forward dip and vanish at large angles. To a certain extent this result still holds for the case of a nucleus consisting of Fermi- particles with common and isobaric spins. In first order only those states can be excited whose wave functions have, in the sense of the independent particle model, a component differing only in the state of one particle from the ground state wave function. In the case of neutron scattering the cross section has a forward dip if the space part of the wave function of the excited particle is orthogonal to the space part of its ground state wave function. If this is not so, for example if the excitation can occur by a pure spin exchange, there may be a forward maximum. In proton scattering the Coulomb interaction could result in a forward peaked angular distribution by didipole excitation as well as in the above mentioned case of monopole transition. In higher approximation two or more particles in the nucleus can be simultaneously excited. The resulting cross sections are expected to be smaller and more isotropic than in the case of a one-particle excitation. The angular distributions for two types of collective excitation have also been calculated, in the first Born approximation, namely for the lowest quadrupole surface vibration and for the dipole vibration of the nuclear charge. The qualitative features of the experimentally measured cross sections of the scattering of 185 MeV protons on C12 are shown to be in agreement with the theoretical expectations." @default.
• W2149756022 created "2016-06-24" @default.
• W2149756022 creator A5006431793 @default.
• W2149756022 creator A5039905790 @default.
• W2149756022 date "1957-03-01" @default.
• W2149756022 modified "2023-10-17" @default.
• W2149756022 title "Inelastic high energy nucleon scattering on light nuclei" @default.
• W2149756022 cites W1996264013 @default.
• W2149756022 cites W2001226755 @default.
• W2149756022 cites W2002975429 @default.
• W2149756022 cites W2006966066 @default.
• W2149756022 cites W2012878246 @default.
• W2149756022 cites W2033301120 @default.
• W2149756022 cites W2035383346 @default.
• W2149756022 cites W2062803276 @default.
• W2149756022 cites W2077618344 @default.
• W2149756022 cites W2087448556 @default.
• W2149756022 cites W2092029305 @default.
• W2149756022 cites W2601319772 @default.
• W2149756022 cites W3019715863 @default.
• W2149756022 doi "https://doi.org/10.1016/0029-5582(57)90050-0" @default.
• W2149756022 hasPublicationYear "1957" @default.
• W2149756022 type Work @default.
• W2149756022 sameAs 2149756022 @default.
• W2149756022 citedByCount "16" @default.
• W2149756022 crossrefType "journal-article" @default.
• W2149756022 hasAuthorship W2149756022A5006431793 @default.
• W2149756022 hasAuthorship W2149756022A5039905790 @default.
• W2149756022 hasConcept C113603373 @default.
• W2149756022 hasConcept C121332964 @default.
• W2149756022 hasConcept C142199849 @default.
• W2149756022 hasConcept C152568617 @default.
• W2149756022 hasConcept C172695262 @default.
• W2149756022 hasConcept C181500209 @default.
• W2149756022 hasConcept C184779094 @default.
• W2149756022 hasConcept C185544564 @default.
• W2149756022 hasConcept C191486275 @default.
• W2149756022 hasConcept C54516573 @default.
• W2149756022 hasConcept C62520636 @default.
• W2149756022 hasConcept C69523127 @default.
• W2149756022 hasConcept C83581075 @default.
• W2149756022 hasConceptScore W2149756022C113603373 @default.
• W2149756022 hasConceptScore W2149756022C121332964 @default.
• W2149756022 hasConceptScore W2149756022C142199849 @default.
• W2149756022 hasConceptScore W2149756022C152568617 @default.
• W2149756022 hasConceptScore W2149756022C172695262 @default.
• W2149756022 hasConceptScore W2149756022C181500209 @default.
• W2149756022 hasConceptScore W2149756022C184779094 @default.
• W2149756022 hasConceptScore W2149756022C185544564 @default.
• W2149756022 hasConceptScore W2149756022C191486275 @default.
• W2149756022 hasConceptScore W2149756022C54516573 @default.
• W2149756022 hasConceptScore W2149756022C62520636 @default.
• W2149756022 hasConceptScore W2149756022C69523127 @default.
• W2149756022 hasConceptScore W2149756022C83581075 @default.
• W2149756022 hasIssue "1" @default.
• W2149756022 hasLocation W21497560221 @default.
• W2149756022 hasOpenAccess W2149756022 @default.
• W2149756022 hasPrimaryLocation W21497560221 @default.
• W2149756022 hasRelatedWork W1017473139 @default.
• W2149756022 hasRelatedWork W2009605494 @default.
• W2149756022 hasRelatedWork W2030295156 @default.
• W2149756022 hasRelatedWork W2031270412 @default.
• W2149756022 hasRelatedWork W2056608202 @default.
• W2149756022 hasRelatedWork W2057804588 @default.
• W2149756022 hasRelatedWork W2065180803 @default.
• W2149756022 hasRelatedWork W2065376163 @default.
• W2149756022 hasRelatedWork W2191432062 @default.
• W2149756022 hasRelatedWork W2883732756 @default.
• W2149756022 hasVolume "3" @default.
• W2149756022 isParatext "false" @default.
• W2149756022 isRetracted "false" @default.
• W2149756022 magId "2149756022" @default.
• W2149756022 workType "article" @default.