Abstract

The contributions from meson exchange and isobar excitation currents to proton-proton bremsstrahlung are discussed within the framework of a relativistic $\mathrm{NN}$ interaction. Below the pion-production threshold the \ensuremath{\Delta} isobar is shown to give the dominant contribution to the two-body currents. The nonrelativistic and static limits to these current operators are discussed, and are shown to give a good approximation to the full relativistic meson-exchange current in the considered kinematic region. For the \ensuremath{\Delta} isobar the static limit is a poor approximation. Including, however, also the energy dependence of the \ensuremath{\Delta} propagation yields a reasonable representation of the isobar excitation current.

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