Surface critical behavior of random systems at the ordinary transition

Abstract

We calculate the surface critical exponents of the ordinary transition occuring in semi-infinite, quenched dilute Ising-like systems. This is done by applying the field theoretic approach directly in d=3 dimensions up to the two-loop approximation, as well as in $d=4-\epsilon$ dimensions. At $d=4-\epsilon$ we extend, up to the next-to-leading order, the previous first-order results of the $\sqrt{\epsilon }$ expansion by Ohno and Okabe [Phys.Rev.B 46, 5917 (1992)]. In both cases the numerical estimates for surface exponents are computed using Pade approximants extrapolating the perturbation theory expansions. The obtained results indicate that the critical behavior of semi-infinite systems with quenched bulk disorder is characterized by the new set of surface critical exponents.

arXiv comment11 pages, 11 figures

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Cited by in corpus (6)

• Critical phenomena at perfect and non-perfect surfaces
• Field theoretical analysis of adsorption of polymer chains at surfaces: Critical exponents and Scaling
• Random field and random anisotropy O(N) spin systems with a free surface
• Surface critical behavior of random systems at the special transition
• Crossover between special and ordinary transitions in random semi-infinite Ising-like systems
• Surface critical behavior of semi-infinite systems with cubic anisotropy at the ordinary transition