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Renormalization-group recursion formulas for magnets with dipolar interactions, derived in previous papers, are generalized to include the case of anisotropic exchange and dipolar forces. For a ferromagnet with a dominant m isotropy (the original spins having n=d=4-ε>m>1 components), the critical exponent ν is 2ν=1+(1/2)(m+2)²ε(m²+10m+12)+O(ε²) [to be compared with 2ν=1+(1/2)(m+2)ε(m+8)+O(ε²) for the pure-exchange case]. For antiferromagnets, the pure-exchange exponents apply.
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Amnon Aharony (1973) studied this question.
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