Tunneling properties in α−T3 lattices: Effects of symmetry-breaking terms

Abstract

The $\ensuremath{\alpha}\text{\ensuremath{-}}{T}_{3}$ lattice model interpolates a honeycomb (graphene-like) lattice and a ${T}_{3}$ (also known as dice) lattice via the parameter $\ensuremath{\alpha}$. These lattices are made up of three atoms per unit cell. This gives rise to an additional dispersionless flat band touching the conduction and valence bands. Electrons in this model are analogous to Dirac fermions with an enlarged pseudospin, which provides unusual tunneling features like omnidirectional Klein tunneling, also called super-Klein tunneling (SKT). However, it is unknown how small deviations in the equivalence between the atomic sites, i.e., variations in the $\ensuremath{\alpha}$ parameter, and the number of tunnel barriers changes the transmission properties. Moreover, it is interesting to learn how tunneling occurs through regions where the energy spectrum changes from linear with a middle flat band to a hyperbolic dispersion. In this paper we investigate these properties, its dependence on the number of square barriers and the $\ensuremath{\alpha}$ parameter for either gapped and gapless cases. Furthermore, we compare these results to the case where electrons tunnel from a region with linear dispersion to a region with a bandgap. In the latter case, contrary to tunneling through a potential barrier, the SKT is no longer observed. Finally, we find specific cases where transmission is allowed due to a symmetry breaking of sublattice equivalence.