A Bipartite Kronig-Penney Model with Dirac Potential Scatterers
arXiv:1903.09159 · doi:10.1088/1361-648X/ab4d67
Abstract
Here we present a simple extension to the age-old Kronig-Penney model, which is made to be bipartite by varying either the scatterer separations or the potential heights. In doing so, chiral (sublattice) symmetry can be introduced. When such a symmetry is present, topologically protected edge states are seen to exist. The solution proceeds through the conventional scattering formalism used to study the Kronig-Penney model, which does not require further tight-binding approximations or mapping into a Su-Schrieffer-Heeger model. The topological invariant for this specific system is found to be the winding of the reflection coefficient, ultimately linked to the system wavefunction. The solution of such a simple and illustrative 1D problem, whose topological content is extracted without requiring further tight-binding approximations, represents the novel aspect of our paper. The cases in which chiral symmetry is absent are then seen to not host topologically protected edge states, as verified by the behaviour of the reflection coefficient and the absence of winding.
arXiv comment15 pages, 16 figures. Noticed crucial typos in equations 8 and 9 leading to a change of figures 5 and 11. The analysis is unchanged however. Change of abstract to better present novel aspects of paper
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