Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physics Letters A

Quantum chaos of the two-level atom

R. Graham, Michael Höhnerbach

Published Mar 1, 1984• 81 citations
Publisher
DOI
10.1016/0375-9601(84)90094-x

Related papers

Quantum Chaos in Atomic two-level and Harmonic Oscillater Systems

稔彦 大野

•Feb 20, 1990•0 citations

Transient Hamiltonian chaos in the interaction of an electromagnetic field with two-level atoms

K. N. Alekseev, G. P. Berman

Journal of Experimental and Theoretical Physics•Mar 1, 1994•3 citations

Quantum aspects of chaos for three-level atoms interacting with two harmonic oscillators

K.D. Harms, Fritz Haake

The European Physical Journal B•Feb 1, 1990•4 citations

Quantum Chaos in Two-Level Systems Interacting with Resonant Radiation Field

Quantum systems of Two-level atoms and radiation which corresponds to semiclassical systems where chaos occurs, are investigated, by using distribution functions obtained fron quantum master equations and its numerical analisis.

•Jan 1, 1988•0 citations

Quantum Chaos in Atomic Physics

Dominique Delande

Springer eBooks•Jul 3, 2007•3 citations

Lyapunov exponents and order-to-chaos transitions in the interaction of two-level atoms with their own radiation field

Leonid E. Kon’kov, Sergey V. Prants

With the help of Lyapunov exponents different routes to quantum chaos are demonstrated numerically in two semiclassical models of the interaction of N two-level atoms with their own radiation field in a resonant cavity. The usual transition to chaos is observed when varying the external control parameter b which describes the interaction of the atomic ensemble with the field. After reaching its critical value b approximately equal to 1 the system becomes more and more chaotic as b increases. As the second control parameter a (the dimensionless individual Rabi frequency) increases the system undergoes transitions to chaos by a completely different way. We observe a complex sequence of order-to-chaos transitions that resembles those for the classical Lorenz attractor.

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE•May 6, 1996•0 citations
With the help of Lyapunov exponents different routes to quantum chaos are demonstrated numerically in two semiclassical models of the interaction of N two-level atoms with their own radiation field in a resonant cavity. The usual transition to chaos is observed when varying the external control parameter b which describes the interaction of the atomic ensemble with the field. After reaching its critical value b approximately equal to 1 the system becomes more and more chaotic as b increases. As the second control parameter a (the dimensionless individual Rabi frequency) increases the system undergoes transitions to chaos by a completely different way. We observe a complex sequence of order-to-chaos transitions that resembles those for the classical Lorenz attractor.