Photo from wikipedia
Differential cross sections of inelastic proton scattering on 13,15C isotopes at energies of 0.6, 0.8, and 1.0 GeV are calculated for levels $${{J}^{{\pi\text{}}}} = {1 \mathord{\left/ {\vphantom {1 {{{2}^{ + }},{5… Click to show full abstract
Differential cross sections of inelastic proton scattering on 13,15C isotopes at energies of 0.6, 0.8, and 1.0 GeV are calculated for levels $${{J}^{{\pi\text{}}}} = {1 \mathord{\left/ {\vphantom {1 {{{2}^{ + }},{5 \mathord{\left/ {\vphantom {5 {{{2}^{ + }}}}} \right. \kern-0em} {{{2}^{ + }}}}}}} \right. \kern-0em} {{{2}^{ + }},{5 \mathord{\left/ {\vphantom {5 {{{2}^{ + }}}}} \right. \kern-0em} {{{2}^{ + }}}}}}$$ in the context of the Glauber multiple scattering theory. Oscillatory wave functions of the shell model are used in the calculations. Partial (first- and second-order) differential cross sections are calculated. It is shown in which range of angles they make the main contributions.
Journal Title: Bulletin of the Russian Academy of Sciences: Physics
Year Published: 2018
Link to full text (if available)
Share on Social Media: Sign Up to like & get
recommendations!