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Trapped ions in laser fields: A benchmark for deformed quantum oscillators (Articolo in rivista)
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- Trapped ions in laser fields: A benchmark for deformed quantum oscillators (Articolo in rivista) (literal)
- Anno
- 2000-01-01T00:00:00+01:00 (literal)
- Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#doi
- 10.1103/PhysRevA.62.053407 (literal)
- Alternative label
Man'ko, V.; Marmo, G.; Porzio, A.; Solimeno, S.; Zaccaria, F. (2000)
Trapped ions in laser fields: A benchmark for deformed quantum oscillators
in Physical review. A; American Physical Society (APS), College Pk (Stati Uniti d'America)
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- Man'ko, V.; Marmo, G.; Porzio, A.; Solimeno, S.; Zaccaria, F. (literal)
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- 1. Univ Naples Federico II, Complesso Univ Monte Sant Angelo, Dipartimento Sci Fis, I-80126 Naples, Italy
2. Ist Nazl Fis Mat, Unita Napoli, I-80138 Naples, Italy
3. Ist Nazl Fis Nucl, Sez Napoli, I-80125 Naples, Italy
4. PN Lebedev Phys Inst, Moscow 1171924, Russia (literal)
- Titolo
- Trapped ions in laser fields: A benchmark for deformed quantum oscillators (literal)
- Abstract
- Some properties of the nonlinear coherent states (NCS), recognized by Vogel and de Mates Filho as dark states of a trapped ion, are extended to NCS on a circle, for which the Wigner functions are presented. These states are obtained by applying a suitable displacement operator D-h(alpha) to the vacuum state. The unity resolutions in terms of the projectors \alpha ,h][alpha ,h(-1)\,\alpha ,h(-1)][alpha ,h\ are presented together with a measure allowing a resolution in terms of \alpha ,h][alpha ,h\. D-h(alpha) is also used for introducing the probability distribution funtion rho (A,h)(z) while the existence of a measure is exploited for extending the P representation to these states. The weight of the nth Fock state of the NCS relative to a trapped ion with Lamb-Dicke parameter eta, oscillates so wildly as n grows up to infinity that the normalized NCS fill the open circle eta (-1) in the complex alpha plane. In addition, this prevents the existence of a measure including normalizable states only. This difficulty is overcome by introducing a family of deformations that are rational functions of n, each of them admitting a measure. By increasing the degree of-these rational approximations, the deformation of a trapped ion can be approximated with any degree of accuracy and the formalism of the P representation can be applied. (literal)
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