TY - JOUR
T1 - Integrability and nonintegrability of quantum systems. II. Dynamics in quantum phase space
AU - Zhang, Wei Min
AU - Feng, Da Hsuan
AU - Yuan, Jian Min
PY - 1990/1/1
Y1 - 1990/1/1
N2 - Based on the concepts of integrability and nonintegrability of a quantum system presented in a previous paper [Zhang, Feng, Yuan, and Wang, Phys. Rev. A 40, 438 (1989)], a realization of the dynamics in the quantum phase space is now presented. For a quantum system with dynamical group scrG and in one of its unitary irreducible-representation carrier spaces gerh, the quantum phase space is a 2M-dimensional topological space, where M is the quantum-dynamical degrees of freedom. This quantum phase space is isomorphic to a coset space scrG/scrH via the unitary exponential mapping of the elementary excitation operator subspace of scrg (algebra of scrG), where scrH (scrG) is the maximal stability subgroup of a fixed state in gerh. The phase-space representation of the system is realized on scrG/scrH, and its classical analogy can be obtained naturally. It is also shown that there is consistency between quantum and classical integrability. Finally, a general algorithm for seeking the manifestation of quantum chaos via the classical analogy is provided. Illustrations of this formulation in several important quantum systems are presented.
AB - Based on the concepts of integrability and nonintegrability of a quantum system presented in a previous paper [Zhang, Feng, Yuan, and Wang, Phys. Rev. A 40, 438 (1989)], a realization of the dynamics in the quantum phase space is now presented. For a quantum system with dynamical group scrG and in one of its unitary irreducible-representation carrier spaces gerh, the quantum phase space is a 2M-dimensional topological space, where M is the quantum-dynamical degrees of freedom. This quantum phase space is isomorphic to a coset space scrG/scrH via the unitary exponential mapping of the elementary excitation operator subspace of scrg (algebra of scrG), where scrH (scrG) is the maximal stability subgroup of a fixed state in gerh. The phase-space representation of the system is realized on scrG/scrH, and its classical analogy can be obtained naturally. It is also shown that there is consistency between quantum and classical integrability. Finally, a general algorithm for seeking the manifestation of quantum chaos via the classical analogy is provided. Illustrations of this formulation in several important quantum systems are presented.
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U2 - 10.1103/PhysRevA.42.7125
DO - 10.1103/PhysRevA.42.7125
M3 - Article
AN - SCOPUS:0000035266
SN - 2469-9926
VL - 42
SP - 7125
EP - 7150
JO - Physical Review A
JF - Physical Review A
IS - 12
ER -