摘要

We explore how a two-mode squeezed vacuum state sech theta e(alpha dagger b dagger tahh theta) |00 > evolves when it undergoes a single-mode amplitude dissipative channel with rate of decay.. We find that in this process not only the squeezing parameter decreases, tanh theta -> e(-kappa t) tanh theta, but also the second-mode vacuum state evolves into a chaotic state exp{b dagger b ln[(1 - e(-2 kappa t)) tanh(2)theta]}. The outcome state is no more a pure state, but an entangled mixed state.