On the basis of the Pad\'e approximant method we deduce from the exact series expansions for the Ising model that the reduced magnetic susceptibility behaves at the critical point as χfcc≈[0.09923(0.101767-w)]5/4, χbcc≈[0.152773(0.1561789-w)]5/4, χsc≈[0.22138(0.218156-w]5/4, χₜ≈[0.2432(2-√3-w)]7/4, χsq≈[0.35724(√2-1-w)]7/4, and χₕ≈[0.4506(1√3-w)]7/4, where w=tanh(J/kT) and the last figure quoted is somewhat uncertain. The spontaneous magnetization is found to behave as (I₀I_∞)fcc≈[12.5(0.664658-z²)]0.3, (I₀I_∞)bcc≈[10.4(0.5326607-z²)]0.3, (I₀I_∞)sc≈[10.9(0.411940-z²)]0.3, where z=exp(-2J/kT) and again the last place quoted is somewhat uncertain. The numbers 5/4 and 7/4 have an error of at most 10^-3, and 0.3 of at most 10^-2. The lattices referred to are fcc, face-centered cubic; bcc, body-centered cubic; sc, simple cubic; t, triangular; sq, simple quadratic; and h, honeycomb.
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George A. Baker (1961) studied this question.
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