Figure 8

Plots of angular distributions of specific states of the projectilelike fragments (PLFs) and targetlike

fragments (TLFs) populated in different transfer reactions and inelastic excitation which were formed in ${}^{12}\mathrm{C}+{}^{93}\mathrm{Nb}$ (a)–(g) and ${}^{13}\mathrm{C}+{}^{93}\mathrm{Nb}$ (h) reactions. The specific states of projectile/PLFs and/or target/TLFs involved in transfer/inelastic scatterings are mentioned in each panel. Filled squares are the experimental data points and dotted/dashed/solid lines are fresco [1] calculations. For (a) solid and dotted lines correspond to B(E2; $2_1^{+}\to 0_1^{+}$) values of 8.800 and $5.429e^2\mathrm{f}{\mathrm{m}}^4$ respectively. For (b), (c), and (h), the population of multiple excited states of ${}^{92}\mathrm{Nb}$ in the energy range up to 500 keV was considered.