The role of core polarization and of the quenching of the leading shell model configuration in stretched spin states is investigated in a case study of the 9- state at 3.522 MeV in 116Sn. With data on five independent observables available, this is the best documented example of a natural parity stretched (yrast) state. The observables are the electron scattering longitudinal and transverse form factors, the proton-scattering cross section and asymmetry, and the proton-stripping cross section on 115In. By introducing a fully microscopic description of the core polarization, it is possible to account quantitatively for all five observables using an effective nucleon-nucleon interaction based on the free t matrix for the proton scattering and...
The strong interaction is not well understood at low energies or for interactions with low momentum ...
On présente des nouvelles données sur le sujet des collisions inélastiques de nucléons polarisés d'é...
The g factors of 11/2− isomers in semimagic 109Sn and 111Sn (isomeric lifetimes τ=2.9(3) ns and τ=14...
The excitation-energy range 3.5-7.2 MeV in the nucleus Sn-116 has been investigated via the proton s...
The excitation-energy range 3.5-7.2 MeV in the nucleus Sn-116 has been investigated via the proton s...
Inelastic electron scattering form factors away from the closed sd -shell are investigated. This inv...
High spin states in "1"0"4Sn were identified in the reaction "5"8Ni("5...
Stretched spin configurations in 116 Sn have been studied via the reactions 116 Sn(~, p'), 116 Sn(e,...
Subsequent to earlier analyses (1989) of elastic and inelastic scattering of polarised protons in te...
Inelastic electron scattering form factors for fp-shell nuclei 42Ca, 44Ca, 46Ti, 48Ti, 50Cr and 54Fe...
The Sn-116(p, t) Sn-114 reaction has been studied in a high-resolution experiment at an incident pro...
High spin states in ${}^{104}\mathrm{Sn}$ were identified in the reaction ${}^{58}\mathrm{Ni}{(}^{50...
The theoretical and experimental status of high energy spin phenomena is summarized, with emphasis o...
A simple theory is presented for core-hole polarization probed by resonant photoemission in a two-st...
The internal spin structure of the neutron, was studied in deep inelastic scattering of longitudinal...
The strong interaction is not well understood at low energies or for interactions with low momentum ...
On présente des nouvelles données sur le sujet des collisions inélastiques de nucléons polarisés d'é...
The g factors of 11/2− isomers in semimagic 109Sn and 111Sn (isomeric lifetimes τ=2.9(3) ns and τ=14...
The excitation-energy range 3.5-7.2 MeV in the nucleus Sn-116 has been investigated via the proton s...
The excitation-energy range 3.5-7.2 MeV in the nucleus Sn-116 has been investigated via the proton s...
Inelastic electron scattering form factors away from the closed sd -shell are investigated. This inv...
High spin states in "1"0"4Sn were identified in the reaction "5"8Ni("5...
Stretched spin configurations in 116 Sn have been studied via the reactions 116 Sn(~, p'), 116 Sn(e,...
Subsequent to earlier analyses (1989) of elastic and inelastic scattering of polarised protons in te...
Inelastic electron scattering form factors for fp-shell nuclei 42Ca, 44Ca, 46Ti, 48Ti, 50Cr and 54Fe...
The Sn-116(p, t) Sn-114 reaction has been studied in a high-resolution experiment at an incident pro...
High spin states in ${}^{104}\mathrm{Sn}$ were identified in the reaction ${}^{58}\mathrm{Ni}{(}^{50...
The theoretical and experimental status of high energy spin phenomena is summarized, with emphasis o...
A simple theory is presented for core-hole polarization probed by resonant photoemission in a two-st...
The internal spin structure of the neutron, was studied in deep inelastic scattering of longitudinal...
The strong interaction is not well understood at low energies or for interactions with low momentum ...
On présente des nouvelles données sur le sujet des collisions inélastiques de nucléons polarisés d'é...
The g factors of 11/2− isomers in semimagic 109Sn and 111Sn (isomeric lifetimes τ=2.9(3) ns and τ=14...