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NEW GENERALIZED COHERENT STATES

A. D. Jannussis, A. Tsonis

Published Jan 1, 2001• 0 citations
OpenAlex

Abstract

Recently Penson and Solomon have constructed a new family of bosons coherent states by using a specially designed function which is a solution of a functional equation dE(q, x)/dx = E(q, qx), with 0 ≤ q ≤ 1 and E(q, 0) = 1. The above authors by using this function in place of the usual exponential and generate now coherent states |q, z > from the vacuum , which are normalized and continuous in their label z. In this paper we use the same procedure of the above authors, but for an other functional equation of the form DqE(q, x) = E(q, x) ,where Dq is the q − dif f erential operator and we obtain new coherent states |q, z > which are more convenient for the q-bosons. Also we will find the solution of the general commutation relation (3.1) and the coherent states of the coherent states of the corresponding annihilation operator.Especially we investigated the coherent states in the isobosonic and genobosonic formulation of Hadronic Mechanics . AMS Subject Classification: 33E99, 42B10.

Related papers

New generalized coherent states

K. A. Penson, A. I. Solomon

We construct a new family of boson coherent states using a specially designed function which is a solution of a functional equation dε(q,x)/dx=ε(q,qx) with 0⩽q⩽1 and ε(q,0)=1. We use this function in place of the usual exponential to generate new coherent states |q,z〉 from the vacuum, which are normalized and continuous in their label z. These states allow the resolution of unity, and a corresponding weight function is furnished by the exact solution of the associated Stieltjes moment problem. They also permit exact evaluation of matrix elements of an arbitrary polynomial given as a normally-ordered function of boson operators. We exemplify this by showing that the photon number statistics for these states is sub-Poissonian. For any q<1 the states |q,z〉 are squeezed; we obtain and discuss their signal to quantum noise ratio. The function ε(q,x) allows a natural generation of multiboson coherent states of arbitrary multiplicity, which is impossible for the usual coherent states. For q=1 all the above results reduce to those for conventional coherent states. Finally, we establish a link with q-deformed bosons.

Journal of Mathematical Physics•May 1, 1999•99 citations

Mittag-Leffler coherent states

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We create a family of boson coherent states using the functions of Mittag-Leffler (ML) E ( z ), ( >0) and their generalizations E , ( z ), ( , >0) instead of exponentials. These states are shown to satisfy the usual requirements of normalizability, continuity in the label and the resolution of unity with a positive weight function. This last quantity is found for arbitrary , >0 as a solution of an associated Stieltjes moment problem. In addition, for = m = 1,2,3 ... and = 1 (corresponding to E m ( z )) we propose and analyse special q -deformations (0< q 1) of the functions E m ( z ) which serve as a tool to define q -deformed coherent states of ML type. We provide the expressions for expectation values of physical quantities for all the above states. We discuss physical properties of these states, noting that they are squeezed. The ML coherent states are sub-Poissonian in nature, whereas the q -deformed ML states can be sub- and super-Poissonian depending on q . All these states are shown to be eigenstates of deformed boson operators whose commutation relations are given.

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Coherent states (CS) for non-Hermitian systems are introduced as eigenstates of pseudo-Hermitian boson annihilation operators. The set of these CS includes two subsets which form bi-normalized and bi-overcomplete system of states. The subsets consist of eigenstates of two complementary lowering pseudo-Hermitian boson operators. Explicit constructions are provided on the example of one-parameter family of pseudo-boson ladder operators. The wave functions of the eigenstates of the two complementary number operators, which form a bi-orthonormal system of Fock states, are found to be proportional to new polynomials, that are bi-orthogonal and can be regarded as a generalization of standard Hermite polynomials.

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A new class of coherent states and it's properties.

Abdlgader Mohamed

The study of coherent states (CS) for a quantum mechanical system has \nreceived a lot of attention. The definition, applications, generalizations of \nsuch states have been the subject of work by researchers. A common starting \npoint of all these approaches is the observation of properties of the original \nCS for the harmonic oscillator. It is well-known that they are described \nequivalently as (a) eigenstates of the usual annihilation operator, (b) from \na displacement operator acting on a fundamental state and (c) as minimum \nuncertainty states. What we observe in the different generalizations proposed \nis that the preceding definitions are no longer equivalent and only some of \nthe properties of the harmonic oscillator CS are preserved. \nIn this thesis we propose to study a new class of coherent states and \nits properties. We note that in one example our CS coincide with the ones \nproposed by Glauber where a set of three requirements for such states has \nbeen imposed. The set of our generalized coherent states remains invariant \nunder the corresponding time evolution and this property is called temporal \nstability. Secondly, there is no state which is orthogonal to all coherent states (the coherent states form a total set). The third property is that we \nget all coherent states by acting on one of these states [¿fiducial vector¿] with \noperators. They are highly non-classical states, in the sense that in general, \ntheir Bargmann functions have zeros which are related to negative regions of \ntheir Wigner functions. Examples of these coherent states with Bargmann \nfunction that involve the Gamma and also the Riemann ¿ functions are represented. \nThe zeros of these Bargmann functions and the paths of the zeros \nduring time evolution are also studied.

•Jan 1, 2011•0 citations

On the Multiboson Coherent State in Deformed Boson Scheme

Atsushi Kuriyama, Constança Providência, João da Providência +2 more

The treatment for the multiboson coherent state is extended for the completeness of the formulation. The basic idea for the extension is presented in terms of expanding the boson space. The MYT boson mapping plays a central role. The resultant multiboson coherent state includes the state obtained in our previous treatment and the form suggests various multiboson coherent states are possible in the deformed boson scheme. 1 typeset using PTPTEX.sty <ver.1.0>Recently, the present authors published four papers 1), 2), 3) concerning the deformed boson scheme including conventional q-deformation in time-dependent variational method. The series of these papers consists of (I), 1) (II), 2) (III) 2) and the short note 3) and, in this series, we discussed various aspects of the q-deformation appearing in the boson coherent state and its generalized form. For example, in (I), 1) a possible form of the multiboson coherent state and its generalization were described. Its treatment is, in some sense, in close connection with that given by Penson and Solomon. 4) However, the treatment in (I) is limited to a certain special boson subspace. In this sense, it is unsatisfactory and to make it complete is the aim of this paper. Further, the present paper gives a generalization of the treatment proposed by the present authors, which is related to a new boson realization in the Lipkin 5), 6) model. In (I), a possible form of the multiboson coherent state, which we denote as |c0〉〉, was defined in the boson space ˜ B composed by the boson operator (˜c, ˜c ∗ ) in the following form:

•Jan 1, 2002•0 citations
Recently Penson and Solomon have constructed a new family of bosons coherent states by using a specially designed function which is a solution of a functional equation dE(q, x)/dx = E(q, qx), with 0 ≤ q ≤ 1 and E(q, 0) = 1. The above authors by using this function in place of the usual exponential and generate now coherent states |q, z > from the vacuum , which are normalized and continuous in their label z. In this paper we use the same procedure of the above authors, but for an other functional equation of the form DqE(q, x) = E(q, x) ,where Dq is the q − dif f erential operator and we obtain new coherent states |q, z > which are more convenient for the q-bosons. Also we will find the solution of the general commutation relation (3.1) and the coherent states of the coherent states of the corresponding annihilation operator.Especially we investigated the coherent states in the isobosonic and genobosonic formulation of Hadronic Mechanics . AMS Subject Classification: 33E99, 42B10.
We construct a new family of boson coherent states using a specially designed function which is a solution of a functional equation dε(q,x)/dx=ε(q,qx) with 0⩽q⩽1 and ε(q,0)=1. We use this function in place of the usual exponential to generate new coherent states |q,z〉 from the vacuum, which are normalized and continuous in their label z. These states allow the resolution of unity, and a corresponding weight function is furnished by the exact solution of the associated Stieltjes moment problem. They also permit exact evaluation of matrix elements of an arbitrary polynomial given as a normally-ordered function of boson operators. We exemplify this by showing that the photon number statistics for these states is sub-Poissonian. For any q<1 the states |q,z〉 are squeezed; we obtain and discuss their signal to quantum noise ratio. The function ε(q,x) allows a natural generation of multiboson coherent states of arbitrary multiplicity, which is impossible for the usual coherent states. For q=1 all the above results reduce to those for conventional coherent states. Finally, we establish a link with q-deformed bosons.
We create a family of boson coherent states using the functions of Mittag-Leffler (ML) E ( z ), ( >0) and their generalizations E , ( z ), ( , >0) instead of exponentials. These states are shown to satisfy the usual requirements of normalizability, continuity in the label and the resolution of unity with a positive weight function. This last quantity is found for arbitrary , >0 as a solution of an associated Stieltjes moment problem. In addition, for = m = 1,2,3 ... and = 1 (corresponding to E m ( z )) we propose and analyse special q -deformations (0< q 1) of the functions E m ( z ) which serve as a tool to define q -deformed coherent states of ML type. We provide the expressions for expectation values of physical quantities for all the above states. We discuss physical properties of these states, noting that they are squeezed. The ML coherent states are sub-Poissonian in nature, whereas the q -deformed ML states can be sub- and super-Poissonian depending on q . All these states are shown to be eigenstates of deformed boson operators whose commutation relations are given.
Coherent states (CS) for non-Hermitian systems are introduced as eigenstates of pseudo-Hermitian boson annihilation operators. The set of these CS includes two subsets which form bi-normalized and bi-overcomplete system of states. The subsets consist of eigenstates of two complementary lowering pseudo-Hermitian boson operators. Explicit constructions are provided on the example of one-parameter family of pseudo-boson ladder operators. The wave functions of the eigenstates of the two complementary number operators, which form a bi-orthonormal system of Fock states, are found to be proportional to new polynomials, that are bi-orthogonal and can be regarded as a generalization of standard Hermite polynomials.
Coherent states (CS) for non-Hermitian systems are introduced as eigenstates of pseudo-Hermitian boson annihilation operators. The set of these CS includes two subsets which form bi-normalized and bi-overcomplete system of states. The subsets consist of eigenstates of two complementary lowering pseudo-Hermitian boson operators. Explicit constructions are provided on the example of one-parameter family of pseudo-boson ladder operators. The wave functions of the eigenstates of the two complementary number operators, which form a bi-orthonormal system of Fock states, are found to be proportional to new polynomials, that are bi-orthogonal and can be regarded as a generalization of standard Hermite polynomials.
The study of coherent states (CS) for a quantum mechanical system has \nreceived a lot of attention. The definition, applications, generalizations of \nsuch states have been the subject of work by researchers. A common starting \npoint of all these approaches is the observation of properties of the original \nCS for the harmonic oscillator. It is well-known that they are described \nequivalently as (a) eigenstates of the usual annihilation operator, (b) from \na displacement operator acting on a fundamental state and (c) as minimum \nuncertainty states. What we observe in the different generalizations proposed \nis that the preceding definitions are no longer equivalent and only some of \nthe properties of the harmonic oscillator CS are preserved. \nIn this thesis we propose to study a new class of coherent states and \nits properties. We note that in one example our CS coincide with the ones \nproposed by Glauber where a set of three requirements for such states has \nbeen imposed. The set of our generalized coherent states remains invariant \nunder the corresponding time evolution and this property is called temporal \nstability. Secondly, there is no state which is orthogonal to all coherent states (the coherent states form a total set). The third property is that we \nget all coherent states by acting on one of these states [¿fiducial vector¿] with \noperators. They are highly non-classical states, in the sense that in general, \ntheir Bargmann functions have zeros which are related to negative regions of \ntheir Wigner functions. Examples of these coherent states with Bargmann \nfunction that involve the Gamma and also the Riemann ¿ functions are represented. \nThe zeros of these Bargmann functions and the paths of the zeros \nduring time evolution are also studied.
The treatment for the multiboson coherent state is extended for the completeness of the formulation. The basic idea for the extension is presented in terms of expanding the boson space. The MYT boson mapping plays a central role. The resultant multiboson coherent state includes the state obtained in our previous treatment and the form suggests various multiboson coherent states are possible in the deformed boson scheme. 1 typeset using PTPTEX.sty <ver.1.0>Recently, the present authors published four papers 1), 2), 3) concerning the deformed boson scheme including conventional q-deformation in time-dependent variational method. The series of these papers consists of (I), 1) (II), 2) (III) 2) and the short note 3) and, in this series, we discussed various aspects of the q-deformation appearing in the boson coherent state and its generalized form. For example, in (I), 1) a possible form of the multiboson coherent state and its generalization were described. Its treatment is, in some sense, in close connection with that given by Penson and Solomon. 4) However, the treatment in (I) is limited to a certain special boson subspace. In this sense, it is unsatisfactory and to make it complete is the aim of this paper. Further, the present paper gives a generalization of the treatment proposed by the present authors, which is related to a new boson realization in the Lipkin 5), 6) model. In (I), a possible form of the multiboson coherent state, which we denote as |c0〉〉, was defined in the boson space ˜ B composed by the boson operator (˜c, ˜c ∗ ) in the following form: