AbstractThe transmissions of fermions are investigated 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 that 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. It is demonstrated 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, it is that introducing a time‐varying potential results in transmissions dispersing across both the central band and the sidebands.