PreprintCC BY 4.0arXiv
Sharp Logarithmic Quantum Dynamics for Quasiperiodic Schrödinger Operators
Abstract
Dynamical localization requires all position moments of a quantum wavepacket to remain bounded in time, but for quasiperiodic Schrödinger operators such bounds are generally not uniform in phase. In the positive Lyapunov exponent regime, the best known phase-uniform estimates instead grow on a logarithmic scale. We prove that both the logarithmic scale and the dependence on the moment order are sharp for a class of one-frequency quasiperiodic Schrödinger operators with even potentials. Our main ingredient is a reflective version of semi-uniformly localized eigenfunctions, adapted to the two localization centers forced by a completely resonant phase, from which we obtain matching logarithmic lower bounds along sequences of times.
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BibTeX
@misc{liu2026sharp,
title = {{Sharp Logarithmic Quantum Dynamics for Quasiperiodic Schrödinger Operators}},
author = {Wencai Liu and Xueyin Wang},
howpublished = {arXiv},
year = {2026},
month = aug,
doi = {10.48550/arxiv.2608.29339},
eprint = {2608.29339},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2608.29339},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Sharp Logarithmic Quantum Dynamics for Quasiperiodic Schrödinger Operators
AU - Wencai Liu
AU - Xueyin Wang
PY - 2026
DA - 2026/08/29
PB - arXiv
DO - 10.48550/arxiv.2608.29339
UR - https://arxiv.org/abs/2608.29339
AB - Dynamical localization requires all position moments of a quantum wavepacket to remain bounded in time, but for quasiperiodic Schrödinger operators such bounds are generally not uniform in phase. In the positive Lyapunov exponent regime, the best known phase-uniform estimates instead grow on a logarithmic scale. We prove that both the logarithmic scale and the dependence on the moment order are sharp for a class of one-frequency quasiperiodic Schrödinger operators with even potentials. Our main ingredient is a reflective version of semi-uniformly localized eigenfunctions, adapted to the two localization centers forced by a completely resonant phase, from which we obtain matching logarithmic lower bounds along sequences of times.
ER -