Quantum dynamical phase transition in a system with many-body interactions
arXiv:cond-mat/0511639 · doi:10.1016/j.ssc.2006.11.001
Abstract
We introduce a microscopic Hamiltonian model of a two level system with many-body interactions with an environment whose excitation dynamics is fully solved within the Keldysh formalism. If a particle starts in one of the states of the isolated system, the return probability oscillates with the Rabi frequency . For weak interactions with the environment we find a slower oscillation whose amplitude decays with a decoherence rate $1/τ_ϕ=1/(2τ_{\mathrm{SE}% })$. However, beyond a finite critical interaction with the environment, , the decoherence rate becomes . The oscillation period diverges showing a \emph{quantum dynamical phase transition}to a Quantum Zeno phase.
5 pages, 3 figures, minor changes, fig.2 modified, added references
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