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Renormalized coupling constants for 3D scalar λφ^4 field theory and pseudo-ε-expansion

Published 2 Jan 2016 in hep-th, cond-mat.soft, cond-mat.stat-mech, hep-lat, and hep-ph | (1601.00148v1)

Abstract: Renormalized coupling constants g_{2k} that enter the critical equation of state and determine nonlinear susceptibilities of the system possess universal values g*{2k} at the Curie point. They are calculated, along with the ratios R{2k} = g_{2k}/g_4{k-1}, for the three-dimensional scalar \lambda\phi4 field theory within the pseudo-\epsilon-expansion approach. Pseudo-\epsilon-expansions for g*_6, g*_8, R*_6, and R*_8 are derived in the five-loop approximation, numerical estimates are presented for R*_6 and R*_8. The higher-order coefficients of the pseudo-\epsilon-expansions for the sextic coupling are so small that simple Pade approximants turn out to be sufficient to yield very good numerical results. Their use gives R*_6 = 1.650 while the most recent lattice estimate is R*_6 = 1.649(2). For the octic coupling pseudo-\epsilon-expansions are less favorable from the numerical point of view. Nevertheless, Pade-Borel resummation leads in this case to R*_8 = 0.890, the number differing only slightly from the values R*_8 = 0.871, R*_8 = 0.857 extracted from the lattice and field-theoretical calculations.

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