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@INPROCEEDINGS{Novotny:811604,
author = {Novotny, Mark and Jin, Fengping and Yuan, Shengjun and
Miyashita, Seiji and De Raedt, Hans and Michielsen, Kristel},
title = {{D}ecoherence and {T}hermalization at {F}inite
{T}emperatures for {Q}uantum {S}ystems},
reportid = {FZJ-2016-04023},
year = {2016},
abstract = {We consider a quantum system $S$ with Hamiltonian ${\cal
H}_S$ coupled via a Hamiltonian ${\cal H}_{SE}$ to a quantum
environment $E$ with Hamiltonian ${\cal H}_E$. We assume the
entirety $S+E$ is in a canonical-thermal state at an inverse
temperature $\beta$. The entirety is a closed quantum system
which evolves via the time-dependent Schr{\”o}dinger
equation with Hamiltonian ${\cal H}={\cal H}_S+{\cal
H}_E+\lambda{\cal H}_{SE}$ where $\lambda$ is the overall
strength of the system-environment coupling. Using both
large-scale simulations and perturbation theory calculations
in $\lambda$, we have studied a measure $\sigma(t)$ for
decoherence and $\delta(t)$ for thermalization of $S$. We
performed large-scale parallel calculations on spin systems
with up to $N=40$ spins in the entirety, with both real-time
and imaginary-time quantum calculations. We performed
perturbation theory calculations about $\lambda=0$ and
fluctuations about the average for the canonical-thermal
ensemble, for both $\sigma$ and $\delta$. We obtained closed
form expressions for both $\sigma$ and $\delta$, in terms of
the free energies of $S$ and $E$. Our perturbation theory
calculations agree very well with our numerical
calculations, at least as long as $\beta\lambda$ is small.},
month = {Jul},
date = {2016-07-18},
organization = {26th IUPAP International conference on
Statistical Physics, Lyon (France), 18
Jul 2016 - 22 Jul 2016},
subtyp = {Other},
cin = {JSC},
cid = {I:(DE-Juel1)JSC-20090406},
pnm = {511 - Computational Science and Mathematical Methods
(POF3-511)},
pid = {G:(DE-HGF)POF3-511},
typ = {PUB:(DE-HGF)24},
url = {https://juser.fz-juelich.de/record/811604},
}