Droplets in the two-dimensional $\ifmmode±\else\textpm\fiJ$ Ising spin glass

By using problem-dependent mappings to computer-science problems and by applying sophisticated algorithms, one can numerically study some important problems much better compared to applying standard approaches, such as Monte Carlo simulations. Here, by using calculations of ground states of suitable perturbed systems, droplets are obtained in two-dimensional ±J spin glasses, which are in the focus of a currently very lively debate. By using a sophisticated matching algorithm, exact ground states of large systems up to L2=2562 spins can be generated. Furthermore, no equilibration or extrapolation to T=0 is necessary. Three different ±J models are studied here: (a) with free boundary conditions, (b) with fixed boundary conditions, and (c) a diluted system wherein a fraction p=0.125 of all bonds is zero. For large systems, the droplet energy shows for all three models a power-law behavior Edpâ¼Lθdpâ² with θdpâ²<0. This is different from the previous studies of domain walls, wherein a convergence to a constant nonzero value (θDW=0) was found. After correcting for the noncompactness of the droplets, the results are likely to be compatible with θdpââ0.29 for all three models. This is in accordance with the Gaussian system wherein θdp=â0.287(4) (νâ3.5 via ν=â1/θdp). Nevertheless, the disorder-averaged spin-spin correlation exponent η is determined here via the probability to have a nonzero-energy droplet, and ηâ0.22 is found for all three models, in contrast to the model with the Gaussian interactions, where η=0 is exact.