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85036305676
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The present calculations differ from 18 26 in that (1) our treatment is more accurate, (2) the specific heat is considered in the two phases, and (3) three values of n are treated
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The present calculations differ from 1826 in that (1) our treatment is more accurate, (2) the specific heat is considered in the two phases, and (3) three values of n are treated.
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46
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85036348319
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D. B. Murray and B. G. Nickel (unpublished). See also appendix of 3
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D. B. Murray and B. G. Nickel (unpublished). See also appendix of 3.
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85036311729
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That is precisely how universal combinations of amplitudes and scaling relations between exponents occur in the field theoretical framework
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That is precisely how universal combinations of amplitudes and scaling relations between exponents occur in the field theoretical framework.
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65
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85036291357
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Only one family of corrections to scaling (controlled by the unique exponent Δ) is accounted for
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Only one family of corrections to scaling (controlled by the unique exponent Δ) is accounted for.
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66
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85036138330
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Or a combination of the two bounds; see Sec. III B
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Or a combination of the two bounds; see Sec. III B.
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67
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85036284370
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Generally speaking this is true, but θ may be nil because there exist systems which do not approach the Ising fixed point along the RG trajectory that links the Gaussian and Ising fixed points. For example, some models may have correction-to-scaling terms strictly different from those accounted for by field theory. Also, some may have “negative” correction-to-scaling terms. See 40
-
Generally speaking this is true, but θ may be nil because there exist systems which do not approach the Ising fixed point along the RG trajectory that links the Gaussian and Ising fixed points. For example, some models may have correction-to-scaling terms strictly different from those accounted for by field theory. Also, some may have “negative” correction-to-scaling terms. See 40.
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68
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85036357547
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The comparison is made easier than with functions having a limited range of applicability
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The comparison is made easier than with functions having a limited range of applicability.
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0000762249
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Phys. Rev. BC. Bervillier, 14, 4964 (1976).
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