Abstract
In the tight-binding random Hamiltonian on Zd, we consider the charge transport induced by an electric potential which varies sufficiently slowly in time, and prove that it is almost surely equal to zero at high disorder. In order to compute the charge transport, we adopt the adiabatic approximation and prove a weak form of adiabatic theorem while there is no spectral gap at the Fermi energy.
Original language | English |
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Pages (from-to) | 917-940 |
Number of pages | 24 |
Journal | Journal of Statistical Physics |
Volume | 97 |
Issue number | 5-6 |
DOIs | |
Publication status | Published - 1999 Dec |
Keywords
- Adiabatic theorem
- Anderson localization
- Charge transport
ASJC Scopus subject areas
- Statistical and Nonlinear Physics
- Mathematical Physics