paper

Zero-temperature spinglass-ferromagnetic transition : scaling analysis of the domain-wall energy

arXiv:1401.6342 · doi:10.1103/PhysRevB.89.184408

Abstract

For the Ising model with Gaussian random coupling of average and unit variance, the zero-temperature spinglass-ferromagnetic transition as a function of the control parameter can be studied via the size- dependent renormalized coupling defined as the domain-wall energy (i.e. the difference between the ground state energies corresponding to AntiFerromagnetic and and Ferromagnetic boundary conditions in one direction). We study numerically the critical exponents of this zero-temperature transition within the Migdal-Kadanoff approximation as a function of the dimension . We then compare with the mean-field spherical model. Our main conclusion is that in low dimensions, the critical stiffness exponent is clearly bigger than the spin-glass stiffness exponent , but that they turn out to coincide in high enough dimension and in the mean-field spherical model. We also discuss the finite-size scaling properties of the averaged value and of the width of the distribution of the renormalized couplings.

v2=final version, 19 pages, 8 figures

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