Critical behavior of interfaces in disordered Potts ferromagnets : statistics of free-energy, energy and interfacial adsorption
arXiv:0711.2878 · doi:10.1103/PhysRevB.77.134416
Abstract
A convenient way to study phase transitions of finite spins systems of linear size is to fix boundary conditions that impose the presence of a system-size interface. In this paper, we study the statistical properties of such an interface in a disordered Potts ferromagnet in dimension within Migdal-Kadanoff real space renormalization. We first focus on the interface free-energy and energy to measure the singularities of the average and random contributions, as well as the corresponding histograms, both in the low-temperature phase and at criticality. We then consider the critical behavior of the interfacial adsorption of non-boundary states. Our main conclusion is that all singularities involve the correlation length appearing in the average free-energy of the interface of dimension , except for the free-energy width that involves the droplet exponent and another correlation length which diverges more rapidly than . We compare with the spin-glass transition in , where is the 'true' correlation length, and where the interface energy presents unconventional scaling with a chaos critical exponent [Nifle and Hilhorst, Phys. Rev. Lett. 68, 2992 (1992)]. The common feature is that in both cases, the characteristic length scale associated with the chaotic nature of the low-temperature phase, diverges more slowly than the correlation length.
v2 : thoroughly rewritten paper with new title, new data and new interpretations (18 pages, 22 figures)