2001
DOI: 10.5488/cmp.4.3.459
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On the Critical Behaviour of Random Anisotropy Magnets: Cubic Anisotropy

Abstract: The critical behaviour of an m -vector model with a local anisotropy axis of random orientation is studied within the field-theoretical renormalization group approach for cubic distribution of anisotropy axis. Expressions for the renormalization group functions are calculated up to the two-loop order and investigated both by an ε = 4 − d expansion and directly at space dimension d = 3 by means of the Padé-Borel resummation. One accessible stable fixed point indicating a 2nd order ferromagnetic phase transition… Show more

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Cited by 11 publications
(27 citation statements)
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“…This picture found its further confirmation by the fixed d approach in the twoloop [75,76,102] and later in the five-loop [77] approximation of the massive scheme. The minimal subtraction scheme corroborates these results.…”
Section: Cubic Distributionmentioning
confidence: 79%
See 1 more Smart Citation
“…This picture found its further confirmation by the fixed d approach in the twoloop [75,76,102] and later in the five-loop [77] approximation of the massive scheme. The minimal subtraction scheme corroborates these results.…”
Section: Cubic Distributionmentioning
confidence: 79%
“…The last degeneracy was observed also for the diluted cubic model [122,123]. This implies a √ ε-expansion [115,116] for the FPs [75,76,102] rather than an ε-expansion. Among the FPs found with the help of the √ ε-expansion, the FP with coordinates w * < 0, y * > 0, u * = v * = 0 is stable.…”
Section: Cubic Distributionmentioning
confidence: 91%
“…In the limiting cases, the obtained results reproduce the known ones. 45,[50][51][52] Unlike the one-loop approximation, where we know the number of solutions, here we solve the system of nonalgebraic equations and thus the number of FPs is un-known in advance. Nevertheless we keep the notation of FPs used in Table II.…”
Section: B Two-loop Approximationmentioning
confidence: 99%
“…subsection 6.1) of the weakly diluted quenched Ising model. The √ ε expansion of the fixed point XVII holds only for m = 2 and is caused by the one-loop degeneracy of the β u , β v , β y functions for w = 0 (c. f. singularity at m = 2 in the ε-expansion of the fixed point IX) 128 .…”
Section: Critical Behaviour Of Stanley Model With Random Anisotropymentioning
confidence: 99%
“…Resummed values of the fixed points and critical exponents for cubic distribution in two-loop approximation for d = 3127,128 .FP m u…”
mentioning
confidence: 99%