% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Grassberger:830226,
author = {Grassberger, Peter},
title = {{C}ritical phenomena on k -booklets},
journal = {Physical review / E},
volume = {95},
number = {1},
issn = {2470-0045},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2017-03800},
pages = {010102},
year = {2017},
abstract = {We define a "k-booklet" to be a set of k semi-infinite
planes with -infinity < x < infinity and y >= 0, glued
together at the edges (the "spine") y = 0. On such booklets
we study three critical phenomena: self-avoiding random
walks, the Ising model, and percolation. For k = 2, a
booklet is equivalent to a single infinite lattice, and for
k = 1 to a semi-infinite lattice. In both these cases the
systems show standard critical phenomena. This is not so for
k >= 3. Self-avoiding walks starting at y = 0 show a
first-order transition at a shifted critical point, with no
power-behaved scaling laws. The Ising model and percolation
show hybrid transitions, i.e., the scaling laws of the
standard models coexist with discontinuities of the order
parameter at y approximate to 0, and the critical points are
not shifted. In the case of the Ising model, ergodicity is
already broken at T = T-c, and not only for T < T-c as in
the standard geometry. In all three models, correlations (as
measured by walk and cluster shapes) are highly anisotropic
for small y.},
cin = {JSC},
ddc = {530},
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)16},
UT = {WOS:000392285800001},
pubmed = {pmid:28208457},
doi = {10.1103/PhysRevE.95.010102},
url = {https://juser.fz-juelich.de/record/830226},
}