Abstract
We quantify the asymptotic vanishing of the ground-state overlap of two non-interacting Fermi gases in d-dimensional Euclidean space in the thermodynamic limit. Given two one-particle Schrödinger operators in finite-volume which differ by a compactly supported bounded potential, we prove a power-law upper bound on the ground-state overlap of the corresponding non-interacting N-Fermion systems. We interpret the decay exponent γ in terms of scattering theory and find γ=π−2∥arcsin|TE/2|∥2HS, where TE is the transition matrix at the Fermi energy E. This exponent reduces to the one predicted by Anderson [Phys. Rev. 164, 352–359 (1967)] for the exact asymptotics in the special case of a repulsive point-like perturbation.
Item Type: | Journal article |
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Form of publication: | Publisher's Version |
Keywords: | Schrödinger operators; Anderson orthogonality; spectral correlations; scattering theory |
Faculties: | Mathematics, Computer Science and Statistics > Mathematics > Analysis, Mathematical Physics and Numerics |
Subjects: | 500 Science > 510 Mathematics |
URN: | urn:nbn:de:bvb:19-epub-37271-5 |
ISSN: | 1664-039X |
Alliance/National Licence: | This publication is with permission of the rights owner freely accessible due to an Alliance licence and a national licence (funded by the DFG, German Research Foundation) respectively. |
Language: | English |
Item ID: | 37271 |
Date Deposited: | 28. Apr 2017, 06:48 |
Last Modified: | 13. Aug 2024, 13:28 |