Squeeze state

A squeeze state 0γ\ket0_\gamma is created with the squeeze operator S(γ)S(\gamma) applied to the ground state

0γ=S(γ)0=e12(γa2γ(a)2)0. \begin{align*} \ket{0}_\gamma = S(\gamma) \ket 0 = e^{-\frac{1}{2} (\gamma\adj a^2 - \gamma (a\adj)^2)} \ket 0. \end{align*}

A squeeze state is a base state of the harmonic oscillator, squeezed in phase space in the direction of the complex number γ\gamma. The figure illustrates a squeeze state compared to the ground state and a coherent state. The squeeze factor γ\gamma in the figure is real, so the state is squeezed in the xx direction.

We can derive the squeeze state by considering a ground state of one oscillator defined by m1,ω1m_1,\omega_1, in another oscillator m2,ω2m_2,\omega_2. This ground state of one oscillator is “squeezed” compared to the ground state of another.