Center-of-mass effects in electromagnetic two-proton knockout reactions

Abstract

The role of center-of mass (CM) effects in the one-body nuclear current in the description of electromagnetically induced two-nucleon knockout reactions is discussed in connection with the problem of the lack of orthogonality between initial bound states and final scattering states obtained by the use of an energy-dependent optical model potential. Results for the cross sections of the exclusive ${}^{16}$O(e,e${}^{\prime }$pp)${}^{14}$C and ${}^{16}$O(${\hat{I}}^3$,pp)${}^{14}$C knockout reactions in different kinematics are presented and discussed. In super-parallel kinematics CM effects produce a strong enhancement of the ${}^{16}$O(e,e${}^{\prime }$pp)${}^{14}$C${}_{g.s.}$ cross section which strongly reduces the destructive interference between the one-body and $\hat{I}”$-current and the sensitivity to the treatment of the $\hat{I}”$-current found in previous work.

9 pages, 5 figures