Quark Condensate from Renormalization Group Optimized Spectral Density

preprint2015arXivOpen access

Abstract

Our renormalization group consistent variant of optimized perturbation, RGOPT, is used to calculate the nonperturbative QCD spectral density of the Dirac operator and the related chiral quark condensate ⟨qˉq⟩\langle \bar q q \rangle, for nf=2n_f=2 and nf=3n_f=3 massless quarks. Sequences of approximations at two-, three-, and four-loop orders are very stable and give ⟨qˉq⟩nf=21/3(2 GeV)=−(0.833−0.845)Λˉ2\langle \bar q q \rangle^{1/3}_{n_f=2}(2\, {\rm GeV}) = -(0.833-0.845) \barΛ_2 , and ⟨qˉq⟩nf=31/3(2 GeV)=−(0.814−0.838)Λˉ3 \langle \bar q q \rangle^{1/3}_{n_f=3}(2\, {\rm GeV}) = -(0.814-0.838) \barΛ_3 where the range is our estimated theoretical error and Λˉnf\barΛ_{n_f} the basic QCD scale in the MSˉ\rm \bar{MS}-scheme. We compare those results with other recent determinations (from lattice calculations and spectral sum rules).

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