Abstract
In this paper, the exact solution and time-evolution operator for the system with a su(1,1)h(4) Hamiltonian are found by making use of Lewis-Riesenfeld quantum theory. The time-evolution operator is then used to derive the Aharonov-Anandan phase. Finally, the noncyclic evolution is discussed with the help of the Aharonov-Anandan phase and the Berry phase is calculated by taking the adiabatic limit.
- Received 8 January 1991
DOI:https://doi.org/10.1103/PhysRevA.44.1485
©1991 American Physical Society