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Holstein polaron in a pseudospin- quantum spin Hall system: first and second order topological phase transitions

arXiv:2408.14367 · doi:10.1103/PhysRevB.110.235432

Abstract

We theoretically propose the occurrence of a quantum spin Hall (QSH) and a second order topological phase transition (TPT) driven by electron-phonon (e-p) coupling in a pseudospin- fermionic system on an - lattice. Our model is formulated in the spirit of the Kane-Mele model modified by the Holstein Hamiltonian. The Lang-Firsov approach is employed to describe polarons reasonably well in the anti-adiabatic (high frequency) limit and to obtain an effective electronic Hamiltonian. It is shown that the system possesses topologically nontrivial phases up to a critical e-p coupling, and are characterized by the helical QSH edge states along with a non-zero invariant for a certain range of . The topological phase vanishes beyond and is accompanied by a bulk gap closing transition at , manifesting a TPT. We observe a more intriguing phenomenon for higher values of , where the system exhibits TPTs supported by two distinct gap closing transitions at and , while a slim region at slightly lower values hosts a semi-metallic signature below . Subsequently, to explore more intricate features, we introduce a time reversal symmetry breaking magnetic field to trigger the formation of a second order topological phase. The magnetic field, by construction causes a boundary dependent gapping out of the edge states, consequently giving rise to robust corner modes in a tailored open boundary conditions. We justify the formation of the higher order phase by employing an appropriate invariant, namely the projected spin Chern number. Finally, we show that the e-p coupling significantly influences the corner modes (and also the real space energy bandstructure), corroborating a higher order TPT as we tune beyond a critical value for a given value of .

18 pages, 18 figures. Comments are welcome

Holstein polaron in a pseudospin-$1$ quantum spin Hall system: first and second order topological phase transitions · wovepaper