2003
DOI: 10.1088/1464-4266/5/5/004
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Squeezing evolution with non-dissipativeSU(1,1) systems

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Cited by 15 publications
(15 citation statements)
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“…whereρ M andρ I are the statistical-mixture and interference parts whose exact forms are given in [17]. As we mentioned above that for the single-mode cat states the origin of the occurrence of the nonclassical effects is in the quantum interference between the components of the states.…”
mentioning
confidence: 99%
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“…whereρ M andρ I are the statistical-mixture and interference parts whose exact forms are given in [17]. As we mentioned above that for the single-mode cat states the origin of the occurrence of the nonclassical effects is in the quantum interference between the components of the states.…”
mentioning
confidence: 99%
“…For instance, coherent states are close to classical states, however, even (odd) coherent states exhibit significant squeezing (sub-Poissonian statistics) and their photon number distributions provide oscillatory behavior. It is worth reminding that the evolution of the Schrödinger-cat states with the single-mode JCM has been treated in [18,19,20,21].…”
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confidence: 99%
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“…The linear dissipative processes in quantum optical systems can be also studied with SU(1, 1) Lie algebra in the framework of the Liouville space formulation [46,47]. Furthermore, beam splitters [48][49][50] interferometers [51], and linear directional couplers [52,53] are successfully described by SU (2) Lie algebra. In these studies the Baker-Campbell-Hausdorff formulas are useful, where in many cases the quantities to be calculated are exponential functions of the generators of the Lie algebras.…”
Section: Application Of Su(1 1) Casimir Operatormentioning
confidence: 99%
“…As studies with driven two-level systems (having only bound states) show [13][14][15][16], the qualitative properties of the HHG spectra can be calculated analytically us-ing traditional quantum optical notions like e.g., dressed states. An appropriately generalized version of the Jaynes-Cummings-Paul model has also been used to describe high-field, multiphoton processes [17][18][19]. Although a strong analogy can be drawn between the dynamics of a driven two-level system and the three-step model [20], for the realistic description of HHG in gas samples (with the obvious involvement of continuum states), the latter one became more widely used.…”
Section: Introductionmentioning
confidence: 99%