4.6 Article

Iterated projected position algorithm for constructing exponentially localized generalized Wannier functions for periodic and nonperiodic insulators in two dimensions and higher

Journal

PHYSICAL REVIEW B
Volume 103, Issue 7, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.103.075125

Keywords

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Funding

  1. National Science Foundation [DMS-2012286]
  2. Department of Energy [DE-SC0019449]
  3. National Science Foundation Graduate Research Fellowship [DGE-1644868]

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In this study, the problem of calculating exponentially localized generalized Wannier functions in various systems is addressed and the Iterated Projected Position (IPP) algorithm is introduced as a solution. Numerical experiments demonstrate the efficacy of the IPP algorithm in computing exponentially localized bases for different models.
Localized bases play an important role in understanding electronic structure. In periodic insulators, a natural choice of localized basis is given by the Wannier functions which depend on a choice of unitary transform known as a gauge transformation. Over the past few decades, there have been many works that have focused on optimizing the choice of the gauge so that the corresponding Wannier functions are maximally localized or reflect some symmetry of the underlying system. In this work, we consider fully nonperiodic materials where the usual Wannier functions are not well defined and gauge optimization is impractical. To tackle the problem of calculating exponentially localized generalized Wannier functions in both periodic and nonperiodic systems, we discuss the 'iterated projected position (IPP) algorithm. The IPP algorithm is based on matrix diagonalization and therefore unlike optimization-based approaches, it does not require initialization and cannot get stuck at a local minimum. Furthermore, the IPP algorithm is guaranteed by a rigorous analysis to produce exponentially localized functions under certain mild assumptions. We numerically demonstrate that the IPP algorithm can be used to calculate exponentially localized bases for the Haldane model, the Kane-Mele model (in both Z(2) invariant even and Z(2) invariant odd phases), and the p(x) + ip(y) model on a quasicrystal lattice.

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