Quantum corrections to the classical model of the atom-field system

• Verfasst von: Ugulava, Archil [VerfasserIn]
• Verfasst von: Mchedlishvili, G. [VerfasserIn]
• Verfasst von: Chkhaidze, S. [VerfasserIn]
• Verfasst von: Chotorlishvili, Levan [VerfasserIn]
• Titel: Quantum corrections to the classical model of the atom-field system
• Verf.angabe: A. Ugulava, G. Mchedlishvili, S. Chkhaidze, and L. Chotorlishvili
• E-Jahr: 2011
• Jahr: 18 October 2011
• Umfang: 8 S.
• Fussnoten: Gesehen am 30.11.2022
• Titel Quelle: Enthalten in: Physical review / E
• Ort Quelle: College Park, Md. : APS, 1993
• Jahr Quelle: 2011
• Band/Heft Quelle: 84(2011), 4, Artikel-ID 046606, Seite 1-8
• ISSN Quelle: 1550-2376
• DOI: doi:10.1103/PhysRevE.84.046606
• Datenträger: Online-Ressource
• Sprache: eng
• K10plus-PPN: 1824044372

Abstract

The nonlinear-oscillating system in action-angle variables is characterized by the dependence of frequency of oscillation ω(I) on action I. Periodic perturbation is capable of realizing in the system a stable nonlinear resonance at which the action I adapts to the resonance condition ω(I0)≃ω, that is, “sticking” in the resonance frequency. For a particular physical problem there may be a case when I≫ℏ is the classical quantity, whereas its correction ΔI≃ℏ is the quantum quantity. Naturally, dynamics of ΔI is described by the quantum equation of motion. In particular, in the moderate nonlinearity approximation ɛ≪(dω/dI)(I/ω)≪1/ɛ, where ɛ is the small parameter, the description of quantum state is reduced to the solution of the Mathieu-Schrödinger equation. The state formed as a result of sticking in resonance is an eigenstate of the operator ΔˆI that does not commute with the Hamiltonian ˆH. Expanding the eigenstate wave functions in Hamiltonian eigenfunctions, one can obtain a probability distribution of energy level population. Thus, an inverse level population for times lower than the relaxation time can be obtained.