A. Reisman, M. Berkenblit, et al.
JES
The Holstein-Peierls model for a dimer is a very simple description of a tight-binding electron (or exciton) coupled at each site to an optical phonon. We study this problem in a region of parameter space where the three relevant physical quantities, the hopping integral - |t|, the optical phonon frequency Ω and the electron-phonon coupling constant g are of comparable magnitude. We obtain a non-perturbative solution by using a unitary transformation and a variational ansatz in terms of squeezed phonon states. The polaron effective mass behaves very differently at the boundaries of the tight-binding band. We also calculate the mean square amplitudes of the relevant phonon momentum and position variables for our solution. © 1998 Elsevier Science B.V. All rights reserved.
A. Reisman, M. Berkenblit, et al.
JES
E. Burstein
Ferroelectrics
Elizabeth A. Sholler, Frederick M. Meyer, et al.
SPIE AeroSense 1997
I.K. Pour, D.J. Krajnovich, et al.
SPIE Optical Materials for High Average Power Lasers 1992