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We show that (near-)zero energy proton emission from H$_2^+$ in strongtwo-color and broadband laser fields is dominated by a stimulated Ramanscattering process taking place on the electronic ground state. It isfurthermore shown that in the (near-)zero energy region the asymmetry in protonejection induced by asymmetric laser fields is due to the interplay of severalprocesses, rather than only pathway interferences, with vibrational trapping(or bond-hardening) taking a key role.

Zero-energy proton dissociation of H$_2^+$ through stimulated Raman scattering