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@ARTICLE{Popkov:279262,
author = {Popkov, Vladislav and Schadschneider, Andreas and Schmidt,
Johannes and Schütz, Gunter M.},
title = {{F}ibonacci family of dynamical universality classes},
journal = {Proceedings of the National Academy of Sciences of the
United States of America},
volume = {112},
number = {41},
issn = {1091-6490},
address = {Washington, DC},
publisher = {National Acad. of Sciences},
reportid = {FZJ-2015-07277},
pages = {12645 - 12650},
year = {2015},
abstract = {Universality is a well-established central concept of
equilibrium physics. However, in systems far away from
equilibrium, a deeper understanding of its underlying
principles is still lacking. Up to now, a few classes have
been identified. Besides the diffusive universality class
with dynamical exponent z=2, another prominent example is
the superdiffusive Kardar−Parisi−Zhang (KPZ) class with
z=3/2. It appears, e.g., in low-dimensional dynamical
phenomena far from thermal equilibrium that exhibit some
conservation law. Here we show that both classes are only
part of an infinite discrete family of nonequilibrium
universality classes. Remarkably, their dynamical exponents
zα are given by ratios of neighboring Fibonacci numbers,
starting with either z1=3/2 (if a KPZ mode exist) or z1=2
(if a diffusive mode is present). If neither a diffusive nor
a KPZ mode is present, all dynamical modes have the Golden
Mean z=(1+5√)/2 as dynamical exponent. The universal
scaling functions of these Fibonacci modes are asymmetric
Lévy distributions that are completely fixed by the
macroscopic current density relation and compressibility
matrix of the system and hence accessible to experimental
measurement.},
cin = {IAS-2 / ICS-2},
ddc = {000},
cid = {I:(DE-Juel1)IAS-2-20090406 / I:(DE-Juel1)ICS-2-20110106},
pnm = {551 - Functional Macromolecules and Complexes (POF3-551)},
pid = {G:(DE-HGF)POF3-551},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000363130900035},
pubmed = {pmid:26424449},
doi = {10.1073/pnas.1512261112},
url = {https://juser.fz-juelich.de/record/279262},
}