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The European Physical Journal D

Quantum dynamics and decoherence in generalized Coleman-Hepp model and boson detector model

Sachiko Kitajima, C. Takahashi, Fumio Shibata

Published Aug 9, 2004• 9 citations
Publisher
DOI
10.1140/epjd/e2004-00092-4

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Time-evolutions of two-level and multi-level systems in phase relaxation processes are investigated in a systematic way. A general form of the decoherence function which determines phase relaxation of a quantum state is obtained by making use of a microscopic interaction Hamiltonian between the relevant system and reservoir. Furthermore the loss of the phase coherence is described in terms of the Pegg–Barnett phase operator. The decoherence function is explicitly calculated for the stochastic dephasing, the boson detector model and the Coleman–Hepp model.
The modified Coleman-Hepp model proposed recently by Nakazato and Pascazio [Phys. Rev. Lett. 70, 1 (1993)] is further generalized so that an ultrarelativistic particle interacts with a linear array of N spins, each of generic magnitude s rather than 1/2. We study the evolution of an appropriately defined measure C(t) of quantum coherence, with t being time, and elucidate the roles played by N and s on the process of decoherence. It is shown that N and s appear in the form of the product Ns in C(\ensuremath{\infty}) at zero temperature, but not in general. It is also noted that the effect of temperature shows up only for s\ensuremath{\ge}1. We study the temperature dependence of C(\ensuremath{\infty}) in detail, and point out in particular that it is not necessarily a monotonic function of temperature. The limiting cases of s\ensuremath{\rightarrow}\ensuremath{\infty} and/or N\ensuremath{\rightarrow}\ensuremath{\infty} are also considered to investigate how the present model tends to a boson model, that is, a model in which the spins are replaced by harmonic oscillators.