The critical behavior of a system of n-component classical "spins"with anisotropic pair interactions is discussed using renormalization-group techniques for dimension d=4-ε. To first order in ε the correlation and susceptibility exponents in the isotropic limit are 2ν=γ=1+[(n+2)/2(n+8)]ε, while the anisotropy or crossover exponent is φ=1+[n/2(n+8)]ε. When n→∞ these expansions agree with exact spherical-model results. For $n=3$ and $d=3$ series expansions indicate φ1.2 (compared with γ1.38).
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Fisher et al. (1972) studied this question.
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