2011
DOI: 10.1007/s10955-011-0272-1
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Ground States of Two-Dimensional Ising Spin Glasses: Fast Algorithms, Recent Developments and a Ferromagnet-Spin Glass Mixture

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Cited by 26 publications
(21 citation statements)
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“…This part of the integral can be expressed in polar coordinates as ǫ 2 0 2π 0 ρ(r cos θ)ρ(r sin θ)rdrdθ. By substituting from (5) it can be seen easily that the angular part is convergent and the radial part is proportional to ǫ 2(1+µ) . Note that this is actually the probability of having two weak bonds that we discussed above for general w. Nonsingular part of the integral is of order ǫ.…”
Section: Analytical Results For Weak Magnetic Field: Chen-ma Scalingmentioning
confidence: 97%
“…This part of the integral can be expressed in polar coordinates as ǫ 2 0 2π 0 ρ(r cos θ)ρ(r sin θ)rdrdθ. By substituting from (5) it can be seen easily that the angular part is convergent and the radial part is proportional to ǫ 2(1+µ) . Note that this is actually the probability of having two weak bonds that we discussed above for general w. Nonsingular part of the integral is of order ǫ.…”
Section: Analytical Results For Weak Magnetic Field: Chen-ma Scalingmentioning
confidence: 97%
“…By using this approach, large planar spin glasses of up to spins can be treated [ 14 ]. In general, the application of this and similar fast GS algorithms [ 16 ] have been successfully used to clarify the nature of GSs of two-dimensional spin glasses [ 13 , 14 , 17 , 18 , 19 , 20 , 21 , 22 , 23 , 24 , 25 , 26 , 27 , 28 , 29 , 30 , 31 , 32 , 33 , 34 ].…”
Section: Spin Glasses Ground States and Domain Wallsmentioning
confidence: 99%
“…In effect, frustration rules out a GS in which all the bonds are satisfied. As limiting cases one can identify the random bond Ising ferromagnet (FM) as µ → ∞ and the (Gaussian) 2D Edwards Anderson Ising spin glass (SG) [11][12][13] at µ = 0. A GS spin configuration σ GS is simply a minimizer of the energy function Eq.…”
Section: A 2d Random Bond Ising Modelmentioning
confidence: 99%