Abstract
An effective nucleon-nucleon interaction is defined by an optimal fit to select on-and half-off-of-the-energy shell t-and g-matrices determined by solutions of the Lippmann-Schwinger and Brueckner-Bethe-Goldstone equations with the Paris nucleon-nucleon interaction as input. As such, it is seen to better reproduce the interaction on which it is based than other commonly used density dependent effective interactions. The new (medium modified) effective interaction when folded with appropriate density matrices, has been used to define proton-{sup 12}C and proton-{sup 16}O optical potentials. With them elastic scattering data are well fit and the medium effects identifiable. 23 refs., 8 figs.
Citation Formats
Dortmans, P J, and Amos, K.
Density dependent effective interactions.
Australia: N. p.,
1994.
Web.
Dortmans, P J, & Amos, K.
Density dependent effective interactions.
Australia.
Dortmans, P J, and Amos, K.
1994.
"Density dependent effective interactions."
Australia.
@misc{etde_10113763,
title = {Density dependent effective interactions}
author = {Dortmans, P J, and Amos, K}
abstractNote = {An effective nucleon-nucleon interaction is defined by an optimal fit to select on-and half-off-of-the-energy shell t-and g-matrices determined by solutions of the Lippmann-Schwinger and Brueckner-Bethe-Goldstone equations with the Paris nucleon-nucleon interaction as input. As such, it is seen to better reproduce the interaction on which it is based than other commonly used density dependent effective interactions. The new (medium modified) effective interaction when folded with appropriate density matrices, has been used to define proton-{sup 12}C and proton-{sup 16}O optical potentials. With them elastic scattering data are well fit and the medium effects identifiable. 23 refs., 8 figs.}
place = {Australia}
year = {1994}
month = {Dec}
}
title = {Density dependent effective interactions}
author = {Dortmans, P J, and Amos, K}
abstractNote = {An effective nucleon-nucleon interaction is defined by an optimal fit to select on-and half-off-of-the-energy shell t-and g-matrices determined by solutions of the Lippmann-Schwinger and Brueckner-Bethe-Goldstone equations with the Paris nucleon-nucleon interaction as input. As such, it is seen to better reproduce the interaction on which it is based than other commonly used density dependent effective interactions. The new (medium modified) effective interaction when folded with appropriate density matrices, has been used to define proton-{sup 12}C and proton-{sup 16}O optical potentials. With them elastic scattering data are well fit and the medium effects identifiable. 23 refs., 8 figs.}
place = {Australia}
year = {1994}
month = {Dec}
}