  Interband transitions of electrons in a gapped graphene monolayer are highly
stimulated near the Fermi surface when a high-frequency electric wave of weak
intensity and a strong constant electric field are superposed in the plane of
the flake. We consider this phenomenon equivalent to the Franz-Keldysh effect,
paying particular attention to the regime where the photon energy linked to the
fast-oscillating field is just below the graphene gap, so that the quantum
transitions still occur through tunneling effects while being facilitated by
the one-photon absorption channel. In the considered parameter regime the
photo-catalyzed current linked to the described setup is shown to exceed the
one driven by the strong field solely by several orders of magnitude.
Conditions to relieve the impact of the field's finite extension are discussed,
and a formula for the residual current density is derived. The robustness of
our assessment supports the viability of detecting this phenomenon in graphene,
thus providing a simulation of the dynamically-assisted Schwinger mechanism in
QED.
