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Corrections to scaling in the 3D Ising model are studied based on Monte Carlo (MC) simulation results for very large lattices with linear lattice sizes up to L=3456. Our estimated values of the correction-to-scaling exponent ω tend to decrease below the usually accepted value about 0.83 when the smallest lattice sizes, i.e. L<Lmin with Lmin∈[6,64], are discarded from the fits. This behavior apparently confirms some of the known estimates of the Monte Carlo renormalization group (MCRG) method, i.e. ω≈0.7 and ω=0.75(5). We discuss the possibilities that ω is either really smaller than usually expected or these values of ω describe some transient behavior which, eventually, turns into the correct asymptotic behavior at Lmin>64. We propose refining MCRG simulations and analysis to resolve this issue. Our actual MC estimations of the critical exponents η and ν provide stable values η=0.03632(13) and ν=0.63017(31), which well agree with those of the conformal bootstrap method, i.e. η=0.0362978(20) and ν=0.6299709(40).
To determine anomalous dynamic scaling of continuum growth equations, López12 proposed an analytical approach, which is based on the scaling analysis introduced by Hentschel and Family.15 In this work, we generalize this scaling analysis to the (d+1)-dimensional molecular-beam epitaxy equations to determine their anomalous dynamic scaling. The growth equations studied here include the linear molecular-beam epitaxy (LMBE) and Lai–Das Sarma–Villain (LDV). We find that both the LMBE and LDV equations, when the substrate dimension d>2, correspond to a standard Family–Vicsek scaling, however, when d<2, exhibit anomalous dynamic roughening of the local fluctuations of the growth height. When the growth equations exhibit anomalous dynamic scaling, we obtain the local roughness exponents by using scaling relation αloc=α-zκ, which are consistent with the corresponding numerical results.