Abstract

The purposes of this work are (1) to show that the appropriate generalizations of the oscillator algebra permit the construction of a wide set of nonlinear coherent states in unified form and (2) to clarify the likely contradiction between the nonclassical properties of such nonlinear coherent states and the possibility of finding a classical analog for them since they are P-represented by a delta function. In (1) we prove that a class of nonlinear coherent states can be constructed to satisfy a closure relation that is expressed uniquely in terms of the Meijer G-function. This property automatically defines the delta distribution as the P-representation of such states. Then, in principle, there must be a classical analog for them. Among other examples, we construct a family of nonlinear coherent states for a representation of the su(1,1) Lie algebra that is realized as a deformation of the oscillator algebra. In (2), we use a beam splitter to show that the nonlinear coherent states exhibit properties like antibunching that prohibit a classical description for them. We also show that these states lack second-order coherence. That is, although the P-representation of the nonlinear coherent states is a delta function, they are not full coherent. Therefore, the systems associated with the generalized oscillator algebras cannot be considered “classical” in the context of the quantum theory of optical coherence.

Highlights

  • The nonclassical properties of light have received a great deal of attention in recent years, mainly in connection with quantum optics [1], quantum information [2], and the principles of quantum mechanics [3]

  • In this work we propose a modification of the conventional boson algebra that permits the recovering of the majority of the already studied deformed boson algebras as particular cases

  • We have shown that the nonlinear coherent states associated with a series of generalized oscillator algebras can be written in the same mathematical form

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Summary

Introduction

The nonclassical properties of light have received a great deal of attention in recent years, mainly in connection with quantum optics [1], quantum information [2], and the principles of quantum mechanics [3]. The deformed oscillator algebras have been used to construct the corresponding generalized ( called nonlinear) coherent states Most of these states exhibit nonclassical properties that distinguish them from the coherent states of the conventional boson algebra. Following [23, 24], the fields represented by such states would have a classical analog These states have nonclassical properties that can be exhibited either with the help of a beam splitter [25] (see [26]) or by showing that their statistics is sub-Poissonian [4]. We have added an appendix with some important mathematical expressions that are not required for reading the paper but are necessary to follow the calculations

Generalized Oscillators
Nonlinear Coherent States
Hilbert Spaces of Analytic Functions
Does the Completeness of Generalized Coherent States Imply Classicality?
Concluding Remarks
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