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33645076875
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max≈0.542719). The choice of the parameters a,b is not crucial and different choices would perform analogously.
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64
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41349110878
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and references therein
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With our definition of §(β,L) the small-z behavior of F§(z) is determined [49] by the small-momentum behavior of the inverse of the two-point function of the fundamental fields. As in the Ising model without disorder (see V. Martín-Mayor, A. Pelissetto, and E. Vicari, Phys. Rev. E 66, 026112 (2002), and references therein), also in the RIM such corrections are extremely tiny [P. Calabrese, V. Martín-Mayor, A. Pelissetto, and E. Vicari (unpublished)].
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With our definition of §(β,L) the small-z behavior of F§(z) is determined [49] by the small-momentum behavior of the inverse of the two-point function of the fundamental fields. As in the Ising model without disorder (see V. Martín-Mayor, A. Pelissetto, and E. Vicari, Phys. Rev. E 66, 026112 (2002), and references therein), also in the RIM such corrections are extremely tiny [P. Calabrese, V. Martín-Mayor, A. Pelissetto, and E. Vicari (unpublished)].
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In Ref. [26], results are given for the rescaled couplings ū and v̄. The relation is u ≡ 6πū, v ≡ 16πv̄/3
-
-
-
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