Matches in SemOpenAlex for { <https://semopenalex.org/work/W2108778820> ?p ?o ?g. }
- W2108778820 abstract "Abstract Energy spectra up to Ex = 20 MeV and angular distributions of τ-particles from the 15N(d, τ)14C reaction have been measured at an incident energy of 52 MeV and have been analysed by the DWBA. Five strong l = 1 transitions to 1p proton hole states occur up to Ex = 11.29 MeV, which is 3 MeV above the particle emission threshold. The absence of direct l = 0 and l = 2 transitions demonstrates that 15N is a good shell-model nucleus with respect to protons. The isobaric analogue 1p hole states in 14C and 14N are identified by a comparison with T = 1 states excited in the 15N(p, d) reaction. This implies the following assignments for 14C levels: Jπ = 2+ for the 8.32 MeV level; Jπ = 1+ for a new level at 11.29±0.04 MeV with a width of 150±50 keV; Jπ = (0, 1, 2)+ for one of the 10.433 and 10.453 MeV levels. This state corresponds to the formerly unknown T = 1, Tz = 0 isobaric analogue at 12.52 MeV in 14N. The Jπ = 0+ and 1+, T = 1 states of mass 14 are rather pure 1p hole states, while the (2+, 1) states are strongly mixed with (s, d)2 configurations. The complete 1p−2 spectrum could be observed. Combined with neutron pick-up data the six diagonal matrix elements of the 1 p 1 2 −2 and the 1 p 1 2 −1 1 p 3 2 −1 interaction have been determined and compared to theoretical results. The eight multipole coefficients ακτ(j1j2) have been calculated by the use of the energy weighted sum rules. The 1 p 1 2 −1 1 p 3 2 −1 spectrum is nearly identical to one produced by a δ-force without exchange terms." @default.
- W2108778820 created "2016-06-24" @default.
- W2108778820 creator A5009808761 @default.
- W2108778820 creator A5063151391 @default.
- W2108778820 creator A5069398581 @default.
- W2108778820 creator A5075409491 @default.
- W2108778820 creator A5084917911 @default.
- W2108778820 date "1971-12-01" @default.
- W2108778820 modified "2023-09-30" @default.
- W2108778820 title "The 15N(d, τ)14C reaction and high-lying T = 1 states in mass-14 nuclei: A determination of 1p32 diagonal matrix elements" @default.
- W2108778820 cites W1481870410 @default.
- W2108778820 cites W1969130092 @default.
- W2108778820 cites W1973585563 @default.
- W2108778820 cites W1974199226 @default.
- W2108778820 cites W1977325575 @default.
- W2108778820 cites W1977992178 @default.
- W2108778820 cites W1979563754 @default.
- W2108778820 cites W1981831699 @default.
- W2108778820 cites W1983743981 @default.
- W2108778820 cites W1992632872 @default.
- W2108778820 cites W2000905991 @default.
- W2108778820 cites W2006865762 @default.
- W2108778820 cites W2007481153 @default.
- W2108778820 cites W2008560543 @default.
- W2108778820 cites W2017704261 @default.
- W2108778820 cites W2019365424 @default.
- W2108778820 cites W2033156340 @default.
- W2108778820 cites W2035675160 @default.
- W2108778820 cites W2036983642 @default.
- W2108778820 cites W2037120174 @default.
- W2108778820 cites W2060974045 @default.
- W2108778820 cites W2061904689 @default.
- W2108778820 cites W2074806704 @default.
- W2108778820 cites W2078026349 @default.
- W2108778820 cites W2079449508 @default.
- W2108778820 cites W2082415145 @default.
- W2108778820 cites W2314381353 @default.
- W2108778820 cites W2705334828 @default.
- W2108778820 doi "https://doi.org/10.1016/0375-9474(71)90205-3" @default.
- W2108778820 hasPublicationYear "1971" @default.
- W2108778820 type Work @default.
- W2108778820 sameAs 2108778820 @default.
- W2108778820 citedByCount "19" @default.
- W2108778820 countsByYear W21087788202014 @default.
- W2108778820 countsByYear W21087788202015 @default.
- W2108778820 countsByYear W21087788202020 @default.
- W2108778820 crossrefType "journal-article" @default.
- W2108778820 hasAuthorship W2108778820A5009808761 @default.
- W2108778820 hasAuthorship W2108778820A5063151391 @default.
- W2108778820 hasAuthorship W2108778820A5069398581 @default.
- W2108778820 hasAuthorship W2108778820A5075409491 @default.
- W2108778820 hasAuthorship W2108778820A5084917911 @default.
- W2108778820 hasConcept C121332964 @default.
- W2108778820 hasConcept C146211579 @default.
- W2108778820 hasConcept C152568617 @default.
- W2108778820 hasConcept C181500209 @default.
- W2108778820 hasConcept C184779094 @default.
- W2108778820 hasConcept C185544564 @default.
- W2108778820 hasConcept C186370098 @default.
- W2108778820 hasConcept C206191943 @default.
- W2108778820 hasConcept C4839761 @default.
- W2108778820 hasConcept C54516573 @default.
- W2108778820 hasConcept C62520636 @default.
- W2108778820 hasConcept C97355855 @default.
- W2108778820 hasConceptScore W2108778820C121332964 @default.
- W2108778820 hasConceptScore W2108778820C146211579 @default.
- W2108778820 hasConceptScore W2108778820C152568617 @default.
- W2108778820 hasConceptScore W2108778820C181500209 @default.
- W2108778820 hasConceptScore W2108778820C184779094 @default.
- W2108778820 hasConceptScore W2108778820C185544564 @default.
- W2108778820 hasConceptScore W2108778820C186370098 @default.
- W2108778820 hasConceptScore W2108778820C206191943 @default.
- W2108778820 hasConceptScore W2108778820C4839761 @default.
- W2108778820 hasConceptScore W2108778820C54516573 @default.
- W2108778820 hasConceptScore W2108778820C62520636 @default.
- W2108778820 hasConceptScore W2108778820C97355855 @default.
- W2108778820 hasLocation W21087788201 @default.
- W2108778820 hasOpenAccess W2108778820 @default.
- W2108778820 hasPrimaryLocation W21087788201 @default.
- W2108778820 hasRelatedWork W1607001304 @default.
- W2108778820 hasRelatedWork W1965623669 @default.
- W2108778820 hasRelatedWork W1966417066 @default.
- W2108778820 hasRelatedWork W1978793082 @default.
- W2108778820 hasRelatedWork W1987180482 @default.
- W2108778820 hasRelatedWork W1992364314 @default.
- W2108778820 hasRelatedWork W1997201238 @default.
- W2108778820 hasRelatedWork W1997763637 @default.
- W2108778820 hasRelatedWork W2001598637 @default.
- W2108778820 hasRelatedWork W2011448711 @default.
- W2108778820 hasRelatedWork W2019601179 @default.
- W2108778820 hasRelatedWork W2047905520 @default.
- W2108778820 hasRelatedWork W2048173265 @default.
- W2108778820 hasRelatedWork W2058584485 @default.
- W2108778820 hasRelatedWork W2064766849 @default.
- W2108778820 hasRelatedWork W2091015861 @default.
- W2108778820 hasRelatedWork W2091862630 @default.
- W2108778820 hasRelatedWork W2126151192 @default.
- W2108778820 hasRelatedWork W2335453220 @default.
- W2108778820 hasRelatedWork W1965428809 @default.
- W2108778820 isParatext "false" @default.