Finite Size Scaling Analysis of Exact Ground States for +J Spin Glass Models in Two Dimens.pdfVIP
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FiniteSizeScalingAnalysisofExactGroundStatesforJSpinGlassModelsinTwoDimens
Finite Size Scaling Analysis of Exact Ground
States for ±J Spin Glass Models in Two
Dimensions
6
9
9
1 Naoki Kawashima(∗) and Heiko Rieger(∗∗)
c
e
D (∗) Department of Physics, Toho University, Miyama 2-2-1, Funabashi 274, Japan
(∗∗) HLRZ c/o Forschungszentrum J¨ulich, 52425 J¨ulich, Germany
2
1
February 1, 2008
]
n
n PACS. 75.10.Nr, 75.50.Lk, 05.50.+q — Spin Glass, Random Systems, Ising models
-
s
i
d
. Abstract. — With the help of exact ground states obtained by a polynomial algorithm
t
a we compute the domain wall energy ∆ at zero-temperature for the bond-random and the
m site-random Ising spin glass model in two dimensions. We find that in both models the
-
d stability of the ferromagnetic and the spin glass order ceases to exist at a unique con-
n centration pc for the ferromagnetic bonds. In the vicinity of this critical point, the size
o and concentration dependency of the first and second moment of the domain wall energy
c
[ are, for both models, described by a common finite size scaling form. Moreover, below
1 this concentration the stiffness exponent turns out to be slightly negative θS = −0.056(6)
v indicating the absence of any intermediate spin glass phase at non-zero temperature.
6
1
1
2
1 Since Edwards and Anderson (EA) proposed the model for spin glasses, it has been
6 discussed not only among researchers specialized for the subject, but in a rather wide com-
9 munity of physicists working on random systems in general. Perhaps, this is largely because
/
t the EA model is the simplest possible model with short-ranged interaction for which we
a
m might expect a spin glass phase tran
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