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General two-mode squeezed states
Authors:R F Bishop  A Vourdas
Institution:(1) Department of Mathematics, University of Manchester, Institute of Science and Technology, P.O. Box 88, M60 1QD Manchester, UK;(2) Fachbereich Physik, Universität Marburg, Federal Republic of Germany;(3) Present address: Department of Electrical Engineering and Electronics, University of Liverpool, Brownlow Hill, P.O. Box 147, L69 3BX Liverpool, UK
Abstract:The states 
$$\hat \theta $$
|A 1 A 2rang are considered, where the operators 
$$\hat \theta $$
are associated with a unitary representation of the groupSp(4,Ropf), and the two-mode Glauber coherent states |A 1 A 2> are joint eigenstates of the destruction operatorsa 1 anda 2 for the two independent oscillator modes. We show that they are ordinary coherent states with respect to new operatorsb 1 andb 2, which are themselves general linear (Bogolibov) transformations of the original operatorsa 1,a 2 and their hermitian conjugatesa delta 1 ,a delta 2 . We further show how they may be regarded as the most general two-mode squeezed states. Most previous work on two-mode squeezed states appears to be based on more restrictive definitions than our own, and thereby reduces to special cases which are unified within our treatment.
Keywords:
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