2013
DOI: 10.1063/1.4819261
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Quasi-coherent states for damped and forced harmonic oscillator

Abstract: In this study, first we construct the quasi-coherent states for a damped and forced harmonic oscillator and discuss the transition of the system from the damped oscillations to forced steady state oscillations. Second, we generalize the Caldirola-Kanai Hamiltonian into the new systems such as the frequency and the mass parameters are time dependent and discuss three examples of them.

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Cited by 3 publications
(4 citation statements)
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“…with ḟ = df dt , and η = η(t) a complex-valued function that arises by integration. The introduction of ( 15) into (12) gives the energy potential…”
Section: Point Transformationsmentioning
confidence: 99%
See 2 more Smart Citations
“…with ḟ = df dt , and η = η(t) a complex-valued function that arises by integration. The introduction of ( 15) into (12) gives the energy potential…”
Section: Point Transformationsmentioning
confidence: 99%
“…The detailed derivation of equations (11)- (12) in terms of point transformations [55] is as follows. We first consider the explicit dependence of X, τ, and ψ on the set y x t x t , ; , { ( )} given in (8)- (9).…”
Section: Appendix a Point Transformationmentioning
confidence: 99%
See 1 more Smart Citation
“…For this particular case, a constant frequency ω 2 (t) = w 2 1 and a driven force F (t) = A 0 cos(νt), for ν, A 0 ∈ R, are considered. This leads to a forced Caldirola-Kanai oscillator Hamiltonian [10,44] of the form…”
Section: Caldirola-kanai Casementioning
confidence: 99%