We use the generalized Bloch theorem formalism of A. Alase et al. [Phys. Rev. Lett. 117, 076804 (2016)] to analyze simple one-dimensional tight-binding lattice systems connected by Hermitian bonds (all with the same hopping parameter $t$), but containing one bond impurity which can be either Hermitian or non-Hermitian. We calculate the band structure, the bulk-boundary correspondence indicator [$D_L\left(\epsilon \right)$], and analyze the eigenvalues of the lattice translation operator ($z$) for each eigenstate. From the $z$ values the generalized Brillouin zone can be reconstructed. If the impurity is Hermitian (and $\mathcal{PT}$-symmetric), then we find a parameter regime in which two localized edge states separate from the tight-binding band. We then simulate a non-Hermitian impurity by keeping hopping in one direction of the bond impurity the same as the rest of the tight-binding system and varying only its reciprocal. Again, we find a region with localized edge states, but in this case the energy eigenvalues are purely imaginary. We also find that in this case the two zero energy eigenvectors coalesce, hence this system is an exceptional line. We then perform an interpolative scan between the above two scenarios and find that there is an intermediate region exhibiting a non-Hermitian skin effect. In this region a macroscopic fraction of states acquire complex energy eigenvalues and exhibit localization toward the impurity. Our numerical results are supported by a detailed analysis of the solutions of the boundary-impurity equation.

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• Edge states
• Localization
• Skin effect
• Topological materials
• Non-Hermitian systems
• Tight-binding model