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Nucleon isovector charges and twist-2 matrix elements with $N_f=2+1$ dynamical Wilson quarks

Published 3 May 2019 in hep-lat, hep-ph, and nucl-th | (1905.01291v2)

Abstract: We present results from a lattice QCD study of nucleon matrix elements at vanishing momentum transfer for local and twist-2 isovector operator insertions. Computations are performed on gauge ensembles with non-perturbatively improved $N_f=2+1$ Wilson fermions, covering four values of the lattice spacing and pion masses down to $M_\pi\approx200$MeV. Several source-sink separations (typically ~1.0fm to ~1.5fm) allow us to assess excited-state contamination. Results on individual ensembles are obtained from simultaneous two-state fits across all observables and all available source-sink separations with the energy gap as a common fit parameter. Renormalization has been performed non-perturbatively using the Rome-Southampton method for all but the finest lattice spacing for which an extrapolation has been used. Physical results are quoted in the $\overline{MS}$ scheme at a scale of $\mu=2$GeV and are obtained from a combined chiral, continuum and finite-size extrapolation. For the nucleon isovector axial, scalar and tensor charges we find physical values of $g_A{u-d}=1.242(25)\text{stat}(\genfrac{}{}{0pt}{2}{+00}{-31})\text{sys}$, $g_S{u-d}=1.13(11)\text{stat}(\genfrac{}{}{0pt}{2}{+07}{-06})\text{sys}$ and $g_T{u-d}=0.965(38)\text{stat}(\genfrac{}{}{0pt}{2}{+13}{-41})\text{sys}$, respectively, where individual systematic errors in each direction from the chiral, continuum and finite-size extrapolation have been added in quadrature. Our final results for the isovector average quark momentum fraction and the isovector helicity and transversity moments are given by $\langle x\rangle_{u-d}=0.180(25)\text{stat}(\genfrac{}{}{0pt}{2}{+14}{-06})\text{sys}$, $\langle x\rangle_{\Delta u-\Delta d}=0.221(25)\text{stat}(\genfrac{}{}{0pt}{2}{+10}{-00})\text{sys}$ and $\langle x\rangle_{\delta u-\delta d}=0.212(32)\text{stat}(\genfrac{}{}{0pt}{2}{+20}{-10})\text{sys}$, respectively.

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