Abstract

The interplay between higher orders of the perturbative QCD (pQCD) expansion and higher-twist contributions in the analysis of recent Jefferson Lab data on the lowest moment of the spin-dependent proton Γ1p(Q2)Γ_1^{p} (Q^2) at 0.05<Q2<3GeV20.05<Q^2< 3 {\rm GeV}^2 is studied. We demonstrate that the values of the higher-twist coefficients μ2kp,nμ^{p,n}_{2k} extracted from the data by using the singularity-free analytic perturbation theory provide a better convergence of the higher-twist series than with the standard perturbative QCD. From the high-precision proton data, we extract the value of the singlet axial charge a0(1GeV2)=0.33±0.05a_0(1 {\rm GeV}^2)=0.33\pm0.05. We observe a slow Q2Q^2 dependence of fitted values of the twist coefficient μ4μ_4 and a0a_0 when going to lower energy scales, which can be explained by the renormalization group evolution of μ4(Q2)μ_4(Q^2) and a0(Q2)a_0(Q^2). As the main result, a good quantitative description of all the Jefferson Lab data sets down to $Q \simeq 350 MeV is achieved.

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