Exact solution of one class of Maryland model
Quantum Physics
2011-11-10 v5
Abstract
The Hamiltonian H of one-body Maryland model is defined as the sum of a linear unperturbed Hamiltonian H_0 and the interaction V, which is a Toeplitz matrix. Maryland model with a doubly infinite Hilbert space are exactly solved. Special cases of one-body Maryland model include the original Maryland model (Phys. Rev. Lett. 49, 833 (1982) and Physica 10D, 369 (1984)), which describes a quantum kickied linear rotator and single band Bloch oscillations. Maryland model and single band Bloch oscillations are the same Hamiltonian in two different representations. A special case of many-body Maryland model is Luttinger model.
Keywords
Cite
@article{arxiv.0709.2494,
title = {Exact solution of one class of Maryland model},
author = {Tao Ma},
journal= {arXiv preprint arXiv:0709.2494},
year = {2011}
}
Comments
5 pages, no figures