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

Il Nuovo cimento della Società italiana di fisica. B/Il Nuovo cimento B

Oscillations in a system comprisingN two-level molecules and a radiation field

V.F. Chel'tzov

Published Oct 1, 1970• 9 citations
Publisher
DOI
10.1007/bf02710983

Related papers

Oscillations in a System Comprising Two-level Molecules and a Radiation Field

Vladislav Cheltsov

Journal of Experimental and Theoretical Physics•Oct 1, 1965•0 citations

OSCILLATIONS IN A SYSTEM OF TWO-LEVEL MOLECULES AND A RADIATION FIELD

Vladislav Cheltsov

•Apr 1, 1965•0 citations

Higher-order squeezing oscillations of the single-mode cavity field interacting with a three-level radiator

V. I. Koroli, S. A. Palistrant, Andrei Nistreanu

We study the two-photon interaction between a three-level equidistant radiator (atom, molecule) with different dipole transitions and the single-mode cavity field. It is supposed that the three-level radiator is laser cooled and trapped into the ground vibrational state, in which the vibrational quantum number [Formula: see text]. In the proposed two-photon Jaynes–Cummings model (JCM) of a three-level atom at the initial moment [Formula: see text], the quantized cavity field is prepared in the squeezed vacuum state and the three-level radiator in the first excited state [Formula: see text]. By using the exact analytical solution for the state-vector of the coupled atom-field system, the amplitude-squared squeezing of the quantized cavity field is examined as a function of the [Formula: see text] and [Formula: see text] parameters. In this situation, higher-order squeezing has the tendency towards oscillations, but the exact periodicity of these oscillations is violated by the analogy with the second-order squeezing.

International Journal of Quantum Information•Dec 1, 2017•0 citations

Coherent interaction of an ultrashort zero-area laser pulse with a Morse oscillator

Szczepan Chelkowski, André D. Bandrauk

Dissociation probabilities, energy absorption, and ground-state populations are calculated numerically for interaction of a Morse oscillator with a resonant ultrashort (${\mathit{t}}_{\mathit{p}}$${10}^{\mathrm{\ensuremath{-}}12}$ sec) intense laser pulse as a function of intensity and pulse area in order to investigate the sensitivity of coherence phenomena to delocalization and chaos in molecule-radiation field systems. It is concluded that a zero-area pulse can reduce considerably energy absorbed by a molecule as well as dissociation probabilities for intensities below and near the chaotic region. It is found that the two-level model (describing the interaction of light resonant with the ground to first excited level transition) works well up to the intensity ${10}^{12}$ W/${\mathrm{cm}}^{2}$, above which transitions to higher levels must be considered.

Physical Review A•Jun 1, 1990•48 citations

Radiation from a System of Resonant Molecules with Energy-level Scatter

A. I. Alekseev, Viktor Mikhaĭlovich Galit︠s︡kiĭ

Journal of Experimental and Theoretical Physics•Apr 1, 1966•0 citations

Temperature dependent properties of the dynamics of a two-level system interacting with a radiation field

Sergey N. Martynov, Almas F. Sadreev

Physica A Statistical Mechanics and its Applications•Jun 1, 1978•3 citations
We study the two-photon interaction between a three-level equidistant radiator (atom, molecule) with different dipole transitions and the single-mode cavity field. It is supposed that the three-level radiator is laser cooled and trapped into the ground vibrational state, in which the vibrational quantum number [Formula: see text]. In the proposed two-photon Jaynes–Cummings model (JCM) of a three-level atom at the initial moment [Formula: see text], the quantized cavity field is prepared in the squeezed vacuum state and the three-level radiator in the first excited state [Formula: see text]. By using the exact analytical solution for the state-vector of the coupled atom-field system, the amplitude-squared squeezing of the quantized cavity field is examined as a function of the [Formula: see text] and [Formula: see text] parameters. In this situation, higher-order squeezing has the tendency towards oscillations, but the exact periodicity of these oscillations is violated by the analogy with the second-order squeezing.
Dissociation probabilities, energy absorption, and ground-state populations are calculated numerically for interaction of a Morse oscillator with a resonant ultrashort (tp{\mathit{t}}_{\mathit{p}}tp​${10}^{\mathrm{\ensuremath{-}}12}$ sec) intense laser pulse as a function of intensity and pulse area in order to investigate the sensitivity of coherence phenomena to delocalization and chaos in molecule-radiation field systems. It is concluded that a zero-area pulse can reduce considerably energy absorbed by a molecule as well as dissociation probabilities for intensities below and near the chaotic region. It is found that the two-level model (describing the interaction of light resonant with the ground to first excited level transition) works well up to the intensity 1012{10}^{12}1012 W/cm2{\mathrm{cm}}^{2}cm2, above which transitions to higher levels must be considered.