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@ARTICLE{Hijar:1884,
author = {Hijar, H. and Quintana, J. and Sutmann, G.},
title = {{P}robability distributions of {H}amiltonian changes in
linear magnetic systems under discontinuous perturbations},
journal = {Journal of statistical mechanics: theory and experiment},
issn = {1742-5468},
address = {Bristol},
publisher = {IOP Publ.},
reportid = {PreJuSER-1884},
pages = {P05009},
year = {2008},
note = {Record converted from VDB: 12.11.2012},
abstract = {A model for the stochastic evolution of a linear
paramagnetic system in contact with a thermal bath and
subjected to variations in time of an external magnetic
field, H, is presented. Changes in the Hamiltonian of this
system, H-H, defined through the relation (W) over tilde =
integral dH (partial derivative H-H/partial derivative H),
are considered for the special case in which the external
field is varied from an initial to a final value in
discontinuous successive steps. Distribution functions of W,
P-F((W) over tilde) and P-R((W) over tilde), corresponding
to switching on and switching off processes, respectively,
are explicitly calculated. To study the relaxation process,
it is assumed that in between successive variations of the
external field, the system follows a linear Langevin
dynamics in the presence of a constant field. The
dependences of P-F((W) over tilde) and P-R((W) over tilde)
on the number of steps in which the external field changes
from initial to final values as well as on the time rate of
the processes are presented. These distributions are used to
estimate free energy differences between two equilibrium
states via the relations of Jarzynski and Crooks, and it is
verified that these relations yield correct estimations of
the free energy difference. Results of the model are
illustrated firstly, for a system of independent two-level
spins in the thermodynamic limit. Finally, a comparison is
also performed with distributions of (W) over tilde in the
two-dimensional Ising model obtained independently from
numerical simulations, carried out in the paramagnetic phase
and restricted to perturbations that produce a linear
response. A good agreement is found between simulations and
the present calculations.},
keywords = {J (WoSType)},
cin = {JSC},
ddc = {530},
cid = {I:(DE-Juel1)JSC-20090406},
pnm = {Scientific Computing},
pid = {G:(DE-Juel1)FUEK411},
shelfmark = {Mechanics / Physics, Mathematical},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000256454900009},
doi = {10.1088/1742-5468/2008/05/P05009},
url = {https://juser.fz-juelich.de/record/1884},
}