2001
DOI: 10.1088/0305-4470/34/37/321
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The quantum under-, critical- and over-damped driven harmonic oscillators

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Cited by 40 publications
(28 citation statements)
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“…For instance the time dependent linear potential has been treated through the Lewis and Riesenfeld [34] invariant theory [28,29,36], Feynman's path integrals [37][38][39][40][41], time-space transformation methods [42] and others [43,44]. The quantum oscillator with time-dependent mass and frequency has been dealt through the group-theoretical approach [45], unitary transformations [4], the Lewis and Riesenfeld invariant theory [46][47][48].…”
Section: Introductionmentioning
confidence: 99%
“…For instance the time dependent linear potential has been treated through the Lewis and Riesenfeld [34] invariant theory [28,29,36], Feynman's path integrals [37][38][39][40][41], time-space transformation methods [42] and others [43,44]. The quantum oscillator with time-dependent mass and frequency has been dealt through the group-theoretical approach [45], unitary transformations [4], the Lewis and Riesenfeld invariant theory [46][47][48].…”
Section: Introductionmentioning
confidence: 99%
“…In fact, the description of quantized energy for a TDHS, such as (10), is a delicate problem. While some authors [1,3,11,21,22] including ours have investigated quantized energy levels for specific TDHSs, there is another opinion [26,27] that such energy levels do not exist for the case of TDHSs. Hence, explicit demonstrations of the existence of quantized energy levels may be an interesting research topic for further study in the future in this field.…”
Section: Quantized Energymentioning
confidence: 82%
“…Typical examples of TDHSs include a damped harmonic oscillator [1][2][3], a harmonic oscillator driven by a time-varying force [4,5], and a harmonic oscillator with time-dependent parameters such as time-dependent mass [6][7][8][9] and/or frequency [10][11][12]. A powerful method for solving quantum solutions of a TDHS is the invariant operator method [13][14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, the propagator can be expanded as a complete set of eigenfunctions for the Hamiltonian operator. For a quadratic Lagrangian, (22) can be written in the form [11] K …”
Section: K(x2 T2;xltl) Yx(tl)=xlmentioning
confidence: 99%