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Dispersive estimates for Dirac equations in Aharonov-Bohm magnetic fields: massive case
Abstract
We study the dispersive properties of the massive Dirac equation perturbed by an Aharonov-Bohm magnetic field, proving in particular dispersive and Strichartz estimates for the associated flow. This paper is the natural continuation of our previous work in the massless case [3], and the overall structure of the analysis remains similar. The presence of a nonzero mass term, however, breaks the scaling invariance of the equation and introduces new difficulties at several stages of the argument. In particular, the appearance of the spectral thresholds +m and -m leads to a genuinely different low energy regime, which requires a separate analysis of the singular angular component.
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BibTeX
@misc{cacciafesta2026dispersive,
title = {{Dispersive estimates for Dirac equations in Aharonov-Bohm magnetic fields: massive case}},
author = {Federico Cacciafesta and Piero D'Ancona and Zhiqing Yin and Junyong Zhang},
howpublished = {arXiv},
year = {2026},
month = nov,
doi = {10.48550/arxiv.2611.07445},
eprint = {2611.07445},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2611.07445},
}
RIS
TY - UNPB
TI - Dispersive estimates for Dirac equations in Aharonov-Bohm magnetic fields: massive case
AU - Federico Cacciafesta
AU - Piero D'Ancona
AU - Zhiqing Yin
AU - Junyong Zhang
PY - 2026
DA - 2026/11/05
PB - arXiv
DO - 10.48550/arxiv.2611.07445
UR - https://arxiv.org/abs/2611.07445
AB - We study the dispersive properties of the massive Dirac equation perturbed by an Aharonov-Bohm magnetic field, proving in particular dispersive and Strichartz estimates for the associated flow. This paper is the natural continuation of our previous work in the massless case [3], and the overall structure of the analysis remains similar. The presence of a nonzero mass term, however, breaks the scaling invariance of the equation and introduces new difficulties at several stages of the argument. In particular, the appearance of the spectral thresholds +m and -m leads to a genuinely different low energy regime, which requires a separate analysis of the singular angular component.
ER -