Abstract
Electroproduction of two vector mesons with a large rapidity gap between them provides the first feasible selective access to chiral-odd GPDs. The scattering amplitude of the process may be represented as a convolution of an impact factor describing the transition and an amplitude describing the transition, analogously to deeply exclusive electroproduction of a meson, the virtual photon being replaced by a Pomeron. The production of a transversely polarized vector meson selects a chiral-odd GPD in the proton.
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