Abstract

The \ensuremath{\rho}\ensuremath{\pi}\ensuremath{\gamma} and \ensuremath{\omega}\ensuremath{\varepsilon}\ensuremath{\gamma} meson exchange current contributions to the deuteron form factors are calculated in a relativistic quasipotential one-boson-exchange model. Recoil corrections to the two-body EM current operator are kept. It is shown that a substantial reduction of the \ensuremath{\rho}\ensuremath{\pi}\ensuremath{\gamma} graph occurs especially at high momentum transfer as compared to the usual nonrelativistic treatment, where only leading-order terms in p/M are retained. As a consequence, the \ensuremath{\omega}\ensuremath{\varepsilon}\ensuremath{\gamma} contribution becomes also important at high momentum transfer. Using the value for the \ensuremath{\omega}\ensuremath{\varepsilon}\ensuremath{\gamma} coupling constant from a relativistic quark model, the elastic EM form factors are predicted in reasonable accordance with the experimental data.

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