Abstract
We shall consider the Schrödinger operators on \(\mathbb {R}^2\) with random \(\delta \) magnetic fields. Under some mild conditions on the positions and the fluxes of the \(\delta \)-fields, we prove the spectrum coincides with \([0,\infty )\) and the integrated density of states (IDS) decays exponentially at the bottom of the spectrum (Lifshitz tail), by using the Hardy-type inequality by Laptev-Weidl (Oper Theory Adv Appl 108:299–305, 1999). We also give a lower bound for IDS at the bottom of the spectrum.
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Communicated by Jean Bellissard.
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Mine, T., Nomura, Y. Schrödinger Operators with Random \(\delta \) Magnetic Fields. Ann. Henri Poincaré 18, 1349–1369 (2017). https://doi.org/10.1007/s00023-017-0559-0
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DOI: https://doi.org/10.1007/s00023-017-0559-0