Abstract
We clarify that the q-generalization of the simple harmonic oscillator to the Arik–Coon one leads us to obtain two different families of q-coherent states in a Fock representation space of the system. They are eigenstates of unbounded and bounded annihilation operators associated with the Arik–Coon q-oscillator. The first family satisfies the resolution of identity condition on all the complex plane and the second one on a disc in radius \(1/\sqrt{1-q}\). Their positive definite q-measures are different, but in the limit \(q\rightarrow 1\) both of them convert to the measure of well-known coherent states for the simple harmonic oscillator. The first and second families of the q-coherent states are also deformed eigenstates of the bounded and unbounded annihilation operators, respectively. Thus, it is possible to study the statistical properties of both q-coherent states via both bounded and unbounded operators. The nonclassical behaviours of interest in this article are signal-to-quantum noise ratio, sub-Poissonian photon statistics, photon antibunching, quadrature squeezing effect and bipartite entanglement for the two families of the q-coherent states, as well as Hillery-type higher-order squeezing for their corresponding photon-added states.
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18 June 2020
Unfortunately, after publication, we found some misprints in Eur. Phys. J. Plus (2020) 135: 253. We list them here because their number is not few.
Notes
Preparing the figures of this article we have used the following approximations: \(E_{q}((1-q)|z|^2)\cong 1+\sum _{k=1}^{1000}\frac{q^{\frac{k(k-1)}{2}}{(1-q)^k|z|^{2k}}}{\Pi _{l=1}^{k}(1-q^l)}\) and \(e_{q}((1-q)|z|^2)\cong 1+\sum _{k=1}^{1000}\frac{{(1-q)^k|z|^{2k}}}{\Pi _{l=1}^{k}(1-q^l)}\).
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Appendix A: q-exponential functions and q-integral representations of the q-factorial
Appendix A: q-exponential functions and q-integral representations of the q-factorial
For a fixed parameter q, the two different generalizations of exponential function are defined as [42]
where \({(a;q)_n:=(1-a)(1-aq)(1-aq^2)\cdots (1-aq^{n-1})}\). The convergence regions of the q-exponential functions for \(0<q<1\) are \(|x|<\infty \) and \(|x|<1\), respectively. The relation \({e_q(x)}{E_q(-x)}=1\) and the classical limits \(\lim _{q\rightarrow 1} {e_q((1-q)x)}=exp(x)\) and \(\lim _{q\rightarrow 1}{E_q((1-q)x)}=exp(x)\) are readily derived from (A1a) and (A1b). Furthermore, in the case \(|q|<1\), there exists an infinite product expansion as follows [46]
Let us assume that f(x) and g(x) are two arbitrary and continuous functions on the real line. The symmetric and asymmetric q-derivatives \(\widetilde{D}_{q,x}\) and \(D_{q,x}\) are defined as [42]
with the following q-analogues for the Leibniz rule:
Being the inverse operations of the q-derivatives \(\widetilde{D}_{q,x}\) and \({D_{q,x}}\), the q-integrals on the intervals \([0,\infty )\) and [0, c] with c as a positive real number are defined as [41, 46]
For any nonzero complex number n, a q-number as \([n]_q:=\frac{1-q^n}{1-q}\) is associated. Also, the q-factorial is defined as \([0]_q!=1\) and \([n]_q!:=[1]_q [2]_q \cdots [n]_q\) for n as a positive integer number. For \(0<q<1\), the following infinite and finite integral representations are obtained by the above definitions for the q- and \(q^2\)-factorials, respectively [40, 41, 46, 47]
We call the attention of the reader to an important issue: quantum number introduced in [46] is symmetric, and to obtain integral relation (A6a), one should write it in terms of the asymmetric quantum number used in this article. Both of the q-integrals convert to the infinite integral representation of the ordinary factorial as \(q\rightarrow 1\).
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Fakhri, H., Mousavi-Gharalari, S.E. Nonclassical properties of two families of q-coherent states in the Fock representation space of q-oscillator algebra. Eur. Phys. J. Plus 135, 253 (2020). https://doi.org/10.1140/epjp/s13360-020-00265-3
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DOI: https://doi.org/10.1140/epjp/s13360-020-00265-3