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Cooperative Effects in Optical Bistability and Resonance Fluorescence

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Coherence and Quantum Optics IV

Abstract

Cooperative phenomena in far-from-equilibrium open systems are presently the object of an ever increasing interest [1]. At a phenomenological level they are described by a set of nonlinear equations with suitable damping terms. Just the interplay of nonlinearity and dissipation gives rise to a large variety of phenomena. Among them, one of the most interesting possibilities is the appearance of phase transitions in stationary nonequilibrium states.

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References

  1. See e.g. a) P. Glansdorff and I. Prigogine, Thermodynamic Theory of Structure, Stability and Fluctuations (Wiley, New York, 1971). b) Synergetics, ed. by H. Haken ( Teubner, Stuttgart, 1973 ).

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  18. Actually in the experiment of Ref. 5 nonlinear dispersion is dominant over nonlinear absorption. For the sake of simplicity, as in Ref. 4, in the present paper we consider the purely absorptive case.

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  20. Note in Eq. (4.2) that the shift ΩI coincides with that predicted by the one-atom theory [9] in the high intensity limit. Furthermore, for γ11= 2γ1 one sees that 2 Re\( \bar \lambda \) coincides with the width of the sidebands as predicted in Ref. 9.

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Bonifacio, R., Lugiato, L.A. (1978). Cooperative Effects in Optical Bistability and Resonance Fluorescence. In: Mandel, L., Wolf, E. (eds) Coherence and Quantum Optics IV. Springer, Boston, MA. https://doi.org/10.1007/978-1-4757-0665-9_29

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  • DOI: https://doi.org/10.1007/978-1-4757-0665-9_29

  • Publisher Name: Springer, Boston, MA

  • Print ISBN: 978-1-4757-0667-3

  • Online ISBN: 978-1-4757-0665-9

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