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21
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85037218917
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Recently we became aware of the fact that the class of states we have defined in Eq. (1) has been considered from the general point of view of quantum groups by V.I. Man'ko, G. Marmo, F. Zaccaria, and E.C.G. Sudarshan, in Proceedings of the IV Wigner Symposium, edited by N. Atakishiyev, T. Seligman, and K.B. Wolf (World Scientific, Singapore, 1996), pp. 421–428. They have introduced these states, denoted as ``f-coherent states'' in view of the dependence of their properties on the chosen function f̌(ň) in Eq. (1), from a mathematical point of view as a generalization of the q-deformed coherent states;
-
Recently we became aware of the fact that the class of states we have defined in Eq. (1) has been considered from the general point of view of quantum groups by V.I. Man'ko, G. Marmo, F. Zaccaria, and E.C.G. Sudarshan, in Proceedings of the IV Wigner Symposium, edited by N. Atakishiyev, T. Seligman, and K.B. Wolf (World Scientific, Singapore, 1996), pp. 421–428. They have introduced these states, denoted as ``f-coherent states'' in view of the dependence of their properties on the chosen function f̌(ň) in Eq. (1), from a mathematical point of view as a generalization of the q-deformed coherent states;
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22
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36149029891
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However, a physical realization of the f-coherent (or nonlinear coherent) states has not been considered by Man'ko
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for the latter, see L.C. Biedenharn, J. Phys. A 22, L873 (1989). However, a physical realization of the f-coherent (or nonlinear coherent) states has not been considered by Man'ko et al
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Biedenharn, L.C.1
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23
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85037234549
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Note that the description of the ionic motion in the harmonic approximation requires a suitable compensation of the micromotion which can be realized experimentally;
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Note that the description of the ionic motion in the harmonic approximation requires a suitable compensation of the micromotion which can be realized experimentally;
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-
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24
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0000020559
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cf. M. Schubert, I. Siemers, R. Blatt, W. Neuhauser and P.E. Toschek, Phys. Rev. Lett. 68, 3016 (1992) and 12.
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Toschek, P.E.5
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26
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3843151527
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The nonlinear Jaynes-Cummings model introduced in 19 has been confirmed in recent experiments by D.M. Meekhof, C. Monroe, B.E. King, W.M. Itano and D.J. Wineland, Phys. Rev. Lett. 76, 1796 (1996).
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Monroe, C.2
King, B.E.3
Itano, W.M.4
Wineland, D.J.5
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27
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85037178674
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Recently it has been shown that even by inclusion of the micromotion a nonlinear Jaynes-Cummings Hamiltonian can be derived that is similar to that obtained in the harmonic approximation in 19
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Recently it has been shown that even by inclusion of the micromotion a nonlinear Jaynes-Cummings Hamiltonian can be derived that is similar to that obtained in the harmonic approximation in 19.
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28
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0038001895
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for details, see P.J. Bardroff, C. Leichtle, G. Schrade and W. P. Schleich, Acta Phys. Slov. 46, 1 (1996).
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Bardroff, P.J.1
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Schrade, G.3
Schleich, W.P.4
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29
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12044259778
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and dark quantum-superposition states in 9
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Previously, dark squeezed states of motion have been considered by J.I. Cirac, R. Blatt, A.S. Parkins and P. Zoller, Phys. Rev. Lett. 70, 556 (1993), and dark quantum-superposition states in 9.
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Cirac, J.I.1
Blatt, R.2
Parkins, A.S.3
Zoller, P.4
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