Quantum driven dissipative parametric oscillator in a blackbody radiation field
We consider the general open system problem of a charged quantum oscillator con- fined in a harmonic trap, whose frequency can be arbitrarily modulated in time, that interacts with both an incoherent quantized (blackbody) radiation field and with an arbitrary coherent laser field. We assume that the...
- Autores:
- Tipo de recurso:
- Fecha de publicación:
- 2017
- Institución:
- Ministerio de Ciencia, Tecnología e Innovación
- Repositorio:
- Repositorio Minciencias
- Idioma:
- eng
- OAI Identifier:
- oai:repositorio.minciencias.gov.co:20.500.14143/34073
- Acceso en línea:
- http://repositorio.colciencias.gov.co/handle/11146/34073
- Palabra clave:
- Teoría cuántica
Números cuánticos
Modelos matemáticos
Energía mecánica
Teoría atómica
Propiedades termodinámicas
- Rights
- License
- http://purl.org/coar/access_right/c_f1cf
Summary: | We consider the general open system problem of a charged quantum oscillator con- fined in a harmonic trap, whose frequency can be arbitrarily modulated in time, that interacts with both an incoherent quantized (blackbody) radiation field and with an arbitrary coherent laser field. We assume that the oscillator is initially in thermodynamic equilibrium with its environment, a non-factorized initial density matrix of the system and the environment, and that at t 0 the modulation of the frequency, the coupling to the incoherent and the coherent radiation are switched on. The subsequent dynamics, induced by the presence of the blackbody radiation, the laser field, and the frequency modulation, is studied in the framework of the influence functional approach. This approach allows incorporating, in analytic closed formulae, the non- Markovian character of the oscillator-environment interaction at any temperature as well the non-Markovian character of the blackbody radiation and its zero-point fluctuations. Expressions for the time evolution of the covariance matrix elements of the quantum fluctuations and the reduced density-operator are obtained. |
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