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

The study of coherent states (CS) for a quantum mechanical system has received a lot of attention. The definition, applications, generalizations of such states have been the subject of work by researchers. A common starting point of all these approaches is the observation of properties of the ori...

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Main Author: Mohamed, Abdlgader
Other Authors: Vourdas, Apostolos
Language:en
Published: University of Bradford 2013
Subjects:
Online Access:http://hdl.handle.net/10454/5724
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spelling ndltd-BRADFORD-oai-bradscholars.brad.ac.uk-10454-57242019-08-31T03:03:02Z A new class of coherent states and it's properties. Mohamed, Abdlgader Vourdas, Apostolos Coherent states Quantum mechanical system Temporal stability Bargmann function Riemann ¿ functions Gamma function Quantum states The study of coherent states (CS) for a quantum mechanical system has received a lot of attention. The definition, applications, generalizations of such states have been the subject of work by researchers. A common starting point of all these approaches is the observation of properties of the original CS for the harmonic oscillator. It is well-known that they are described equivalently as (a) eigenstates of the usual annihilation operator, (b) from a displacement operator acting on a fundamental state and (c) as minimum uncertainty states. What we observe in the different generalizations proposed is that the preceding definitions are no longer equivalent and only some of the properties of the harmonic oscillator CS are preserved. In this thesis we propose to study a new class of coherent states and its properties. We note that in one example our CS coincide with the ones proposed by Glauber where a set of three requirements for such states has been imposed. The set of our generalized coherent states remains invariant under the corresponding time evolution and this property is called temporal stability. 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 get all coherent states by acting on one of these states [¿fiducial vector¿] with operators. They are highly non-classical states, in the sense that in general, their Bargmann functions have zeros which are related to negative regions of their Wigner functions. Examples of these coherent states with Bargmann function that involve the Gamma and also the Riemann ¿ functions are represented. The zeros of these Bargmann functions and the paths of the zeros during time evolution are also studied. Libyan Cultural Affairs 2013-11-28T17:59:18Z 2013-11-28T17:59:18Z 2013-11-28 2011 Thesis doctoral PhD http://hdl.handle.net/10454/5724 en <a rel="license" href="http://creativecommons.org/licenses/by-nc-nd/3.0/"><img alt="Creative Commons License" style="border-width:0" src="http://i.creativecommons.org/l/by-nc-nd/3.0/88x31.png" /></a><br />The University of Bradford theses are licenced under a <a rel="license" href="http://creativecommons.org/licenses/by-nc-nd/3.0/">Creative Commons Licence</a>. University of Bradford Department of Computing
collection NDLTD
language en
sources NDLTD
topic Coherent states
Quantum mechanical system
Temporal stability
Bargmann function
Riemann ¿ functions
Gamma function
Quantum states
spellingShingle Coherent states
Quantum mechanical system
Temporal stability
Bargmann function
Riemann ¿ functions
Gamma function
Quantum states
Mohamed, Abdlgader
A new class of coherent states and it's properties.
description The study of coherent states (CS) for a quantum mechanical system has received a lot of attention. The definition, applications, generalizations of such states have been the subject of work by researchers. A common starting point of all these approaches is the observation of properties of the original CS for the harmonic oscillator. It is well-known that they are described equivalently as (a) eigenstates of the usual annihilation operator, (b) from a displacement operator acting on a fundamental state and (c) as minimum uncertainty states. What we observe in the different generalizations proposed is that the preceding definitions are no longer equivalent and only some of the properties of the harmonic oscillator CS are preserved. In this thesis we propose to study a new class of coherent states and its properties. We note that in one example our CS coincide with the ones proposed by Glauber where a set of three requirements for such states has been imposed. The set of our generalized coherent states remains invariant under the corresponding time evolution and this property is called temporal stability. 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 get all coherent states by acting on one of these states [¿fiducial vector¿] with operators. They are highly non-classical states, in the sense that in general, their Bargmann functions have zeros which are related to negative regions of their Wigner functions. Examples of these coherent states with Bargmann function that involve the Gamma and also the Riemann ¿ functions are represented. The zeros of these Bargmann functions and the paths of the zeros during time evolution are also studied. === Libyan Cultural Affairs
author2 Vourdas, Apostolos
author_facet Vourdas, Apostolos
Mohamed, Abdlgader
author Mohamed, Abdlgader
author_sort Mohamed, Abdlgader
title A new class of coherent states and it's properties.
title_short A new class of coherent states and it's properties.
title_full A new class of coherent states and it's properties.
title_fullStr A new class of coherent states and it's properties.
title_full_unstemmed A new class of coherent states and it's properties.
title_sort new class of coherent states and it's properties.
publisher University of Bradford
publishDate 2013
url http://hdl.handle.net/10454/5724
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