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(D6) Since ⏐ ⏐ dF (r) dr ⏐ ⏐ = 1 − cos ( 2 π (x0 − r) ) < 1, (0 < x0 − r < 1/4), (D7) x0 is an attractor [61]

Convergence of rn to x0 The convergence of the iteration is examined by introducing the following function: F(r) = r + 1 2π sin ( 2π (x0 − r) ) ( mod 1)

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Shaping Maximally Localized Wannier Functions via Discrete Adiabatic Transport

cond-mat.mtrl-sci · 2026-05-14 · unverdicted · novelty 7.0

A non-variational algorithm constructs maximally localized Wannier functions by treating discrete adiabatic transport across band degeneracies as part of solving the projected position operator eigenvalues, yielding linear phase overlaps and fixed-point extraction of centers.

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  • Shaping Maximally Localized Wannier Functions via Discrete Adiabatic Transport cond-mat.mtrl-sci · 2026-05-14 · unverdicted · none · ref 17

    A non-variational algorithm constructs maximally localized Wannier functions by treating discrete adiabatic transport across band degeneracies as part of solving the projected position operator eigenvalues, yielding linear phase overlaps and fixed-point extraction of centers.