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@ARTICLE{Jin:133045,
author = {Jin, Fengping and Michielsen, Kristel and Novotny, Mark A.
and Miyashita, Seiji and Yuan, Shengjun and De Raedt, Hans},
title = {{Q}uantum decoherence scaling with bath size: {I}mportance
of dynamics, connectivity, and randomness},
journal = {Physical review / A},
volume = {87},
number = {2},
issn = {1050-2947},
address = {College Park, Md.},
publisher = {APS},
reportid = {FZJ-2013-01609},
pages = {022117},
year = {2013},
abstract = {We consider the decoherence of a quantum system S coupled
to a quantum environment E. For states chosen uniformly at
random from the unit hypersphere in the Hilbert space of the
closed system S+E we derive a scaling relationship for the
sum of the off-diagonal elements of the reduced density
matrix of S as a function of the size DE of the Hilbert
space of E. This sum decreases as 1/√DE as long as DE≫1.
We test this scaling prediction by performing large-scale
simulations which solve the time-dependent Schrödinger
equation for a ring of spin-1/2 particles, four of them
belonging to S and the others to E, and for this ring with
small world bonds added in E and/or between S and E. The
spin-1/2 particles experience nearest-neighbor interactions
that are identical for the interactions within S and random
for the interactions within E and between S and E, or that
are all identical. Provided that the time evolution drives
the whole system from the initial state toward a scaling
state, a state which has similar properties as states
belonging to the class of quantum states for which we
derived the scaling relationship, the scaling prediction
holds. We examine various interaction parameters and initial
states for our model system to find whether or not the time
evolution reaches the class of states that have the scaling
property. For the homogeneous ring we find that the
evolution for select initial states does not reach these
scaling states. This conclusion is not modified if we add
some homogeneous random connections. For a ring we find that
some randomness in the interaction parameters is required so
that most initial configurations are driven toward the
scaling state. Furthermore, if the amount of randomness is
small the time required to reach the scaling states may be
very large. For the case of all random interactions in E the
ring is driven toward the scaling state. Adding small world
bonds between S and E with random interaction strengths may
decrease the time required to reach the scaling state or may
prevent the scaling state from being reached. For the latter
case we show that increasing the complexity of the
environment by adding extra connections within the
environment suffices to observe the predicted scaling
behavior.},
cin = {JSC},
ddc = {530},
cid = {I:(DE-Juel1)JSC-20090406},
pnm = {411 - Computational Science and Mathematical Methods
(POF2-411)},
pid = {G:(DE-HGF)POF2-411},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000315143200002},
doi = {10.1103/PhysRevA.87.022117},
url = {https://juser.fz-juelich.de/record/133045},
}