Abstract
The squeezed states of two-mode boson systems are defined through canonical transformation. The defined concept of squeezed boson systems has been applied the Hamiltonian H = γ S z 2 − B S x . The ground-state energy of boson systems is investigated by means of squeezed states. We analyze coherent and squeezed Hamiltonian in the group-theoretic method. It is found that squeezing acts as asymmetry breaking.
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