We show that the technique of integration within an ordered product (IWOP) of operators provides us with an approach for deriving the disentangling of the multimode boson realization of SU(1,1) coset element. A new type of generalized squeezed states can thus be constructed.
We have constructed the multimode bosonic realization of the su(1,1) Lie algebra, on the basis of which the su(1,1) generalized coherent state in the multimode Fock space is derived. It is shown that the multimode coherent state is, in fact, the generalized multimode squeezed vacuum state discussed by Lo and Sollie [Phys. Rev. A 47, 733 (1993)], and that the unitary displacement operator can be identified as the generalized multimode squeezing operator. Hence, similar to the single- and two-mode cases, our multimode bosonic realization of the su(1,1) Lie algebra has immediate relevance to the squeezing properties of boson fields.
In this paper we have constructed the multiparticle ( q, p )-realization of the su (1, 1) Lie algebra, and studied its relation to the multimode bosonic realization and squeezing properties. We believe that this multiparticle realization should be very useful in the study of a system of coupled general time-dependent quantum oscillators whose Hamiltonian can be written as a linear combination of the three su (1, 1) generators; in particular, it is more capable to give a vivid picture of the system in the configuration space.
By constructing a generalized multi-partite entangled state representation and introducing the ket-bra integral in this representation, we find a new set of generalized bosonic realization of the generators of the SU (1, 1) algebra, which can compose a generalized multi-mode squeezing operator. This operator squeezes the multi-partite entangled state in a natural way. Then the corresponding multi-mode squeezed vacuum states | r ⟩ is obtained. Based on this, the variances of the n -mode quadratures and the higher-order squeezing in | r ⟩ are evaluated. In addition, we examine the violation of the Bell inequality for | r ⟩ by using the formalism of Wigner representation.