Quasi-free proton-proton scattering in light nuclei at 460 MeV

Neutron scattering from28Si and32S from 8.0 to 18.9 MeV, dispersive optical model analyses, and ground-state correlations

“…Note that we organized the E nlj data, culled from Refs. [56][57][58][59][60], into two columns labeled ExpA and ExpB. Comparison of our DOM predictions of E nlj to experimental data shows mixed results.…”

Theory of Overlap Functions. I. Single Particle Sum Rules and Centre-of- Mass Corrections.

“…(,r·,1) 9 9 1, T« 1 = -1 L AT·r T J (26) The alternative sets of equations (24) or (25) The above equations immediately generalise these results for a nucleus with non-zero spin and for excited states of the A-particle nucleus.…”

“…However, it is 26,27) unfortunately apparent that present analyses of the data cannot distinguish between the two values. One might possibly use the improved theoretical value as an aid in making more refined analyses.…”

“…Two of the most recent analyses of such experiments have been by Tyrin et.al. 26) and Jain and Jackson . Let us assume that these nuclei ranging between 27) 6 16 Li and 0 have a closed 1sl/2 shell so that S-(ls) = 2 to zero order.…”

Chemistry Division Annual Report, July 1970--June 1971.

“…To remedy these defects calculations were made [28] of d 3 a/dS2 1 dS2 2 dE 1 for individual target nuclear shells for the (p,2p) reactions on 12 C, 16 0, and 40 Ca at 460 MeV and were compared with experiment [29]. The DWIA was used along with the more realistic Woods-Saxon radial wavefunction and a more realistic form of the distorted wavefunction.…”