Abstract
We propose to extend the concept of geometric phase to quantum dissipative systems, in the case of meta-stable spin states in magnetic resonance. We use the generalized version of Lewis–Riensenfeld invariant theory to study the dissipative systems described by non-hermitian time-dependent Hamiltonian.
Information
Published: 1 January 2006
First available in Project Euclid: 13 July 2015
zbMATH: 1098.81043
MathSciNet: MR2228364
Digital Object Identifier: 10.7546/giq-7-2006-79-88
Rights: Copyright © 2006 Institute of Biophysics and Biomedical Engineering, Bulgarian Academy of Sciences
