  We investigate the transmissions of fermions through gapped graphene
structures by employing a combination of double barrier tilting and a
time-oscillating potential. The latter introduces additional sidebands into the
transmission probability, which manifest at energy levels determined by the
frequency and incident energy. These sidebands arise from the absorption or
emission of photons generated by the oscillating potential. We demonstrate that
the tilting and positioning of the scattering events within the barriers play a
crucial role in determining the peak of tunneling resistance. In particular,
the presence of a mid-barrier-embedded scatter leads to a transition from a
peak to a cusp when the incident energy reaches the Dirac point within a
barrier. Additionally, we illustrate that introducing a time-varying potential
results in transmissions dispersing across both the central band and the
sidebands.
