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Recent progress in hadron structure from Lattice QCD

Martha Constantinou

TL;DR

This paper surveys recent progress in hadron structure from lattice QCD, focusing on nucleon matrix elements, axial and tensor charges, and the spin decomposition, including disconnected contributions. It highlights advances enabling simulations near physical pion masses, nonperturbative renormalization, and innovative direct approaches to PDFs through quasi-distributions, as well as gluon moments and the neutron EDM. Key findings include $g_A$ values at the physical point that approach experimental data, consistent $g_T$ results across lattice setups, partial progress in determining gluon momentum fractions, and viable strategies for extracting PDFs from lattice data. The work underscores significant progress toward first-principles predictions to guide experiments and constrain beyond-the-Standard-Model physics, while acknowledging challenges in noise control, operator mixing, and continuum extrapolation.

Abstract

We review recent progress in hadron structure using lattice QCD simulations, with main focus in the evaluation of nucleon quantities such as the axial and tensor charges, and the spin con- tent of the nucleon, using simulations at pion masses close to the physical value. We highlight developments on the evaluation of the gluon moment, a new direct approach to compute quark parton distributions functions on the lattice, as well as, the neutron electric dipole moment. A discussion of the systematic uncertainties and the computation of the disconnected contributions using dynamical simulations is also included.

Recent progress in hadron structure from Lattice QCD

TL;DR

This paper surveys recent progress in hadron structure from lattice QCD, focusing on nucleon matrix elements, axial and tensor charges, and the spin decomposition, including disconnected contributions. It highlights advances enabling simulations near physical pion masses, nonperturbative renormalization, and innovative direct approaches to PDFs through quasi-distributions, as well as gluon moments and the neutron EDM. Key findings include values at the physical point that approach experimental data, consistent results across lattice setups, partial progress in determining gluon momentum fractions, and viable strategies for extracting PDFs from lattice data. The work underscores significant progress toward first-principles predictions to guide experiments and constrain beyond-the-Standard-Model physics, while acknowledging challenges in noise control, operator mixing, and continuum extrapolation.

Abstract

We review recent progress in hadron structure using lattice QCD simulations, with main focus in the evaluation of nucleon quantities such as the axial and tensor charges, and the spin con- tent of the nucleon, using simulations at pion masses close to the physical value. We highlight developments on the evaluation of the gluon moment, a new direct approach to compute quark parton distributions functions on the lattice, as well as, the neutron electric dipole moment. A discussion of the systematic uncertainties and the computation of the disconnected contributions using dynamical simulations is also included.

Paper Structure

This paper contains 11 sections, 32 equations, 11 figures.

Figures (11)

  • Figure 1: Connected (left) and disconnected (right) contributions to the nucleon three-point function.
  • Figure 2: Collection of lattice results for $g_A$ corresponding to: $N_f{=}2{+}1$ DWF (RBC/UKQCD Yamazaki:2008pyYamazaki:2009zq, RBC/UKQCD Ohta:2013qda, $\chi$QCD chiQCD14), $N_f{=}2{+}1$ DWF on asqtad sea (LHPC Bratt:2010jn), $N_f{=}2$ TMF (ETMC Alexandrou:2010hf), $N_f{=}2$ Clover (QCDSF/UKQCD Pleiter:2011gw, CLS/MAINZ Capitani:2012gj, QCDSF Horsley:2013ayv, RQCD Bali:2014nma), $N_f{=}2{+}1$ Clover (LHPC Green:2012rr, CSSM Owen:2012ts), $N_f{=}2{+}1{+}1$ TMF (ETMC Alexandrou:2013joa), $N_f{=}2{+}1{+}1$ HISQ (PNDME Bhattacharya:2013ehcPNDME14), $N_f{=}2$ TMF with Clover (ETMC Abdel-Rehim:2015owa). The asterisk is the experimental value PDG12.
  • Figure 3: Lattice results for $g_T$ as a function of the $m_\pi^2$, corresponding to: $N_f{=}2$ Clover (QCDSF/UKQCD Gockeler:2005cjPleiter:2011gwBali:2014nma), $N_f{=}2$ DWF (RBC Lin:2008uz), $N_f{=}2{+}1$ DWF (RBC/UKQCD Ohta:2008kdAoki:2010xg, LHPC Green:2012ej), $N_f{=}2{+}1$ DWF on asqtad sea (LHPC Bratt:2010jnGreen:2012ej), $N_f{=}2{+}1$ Clover (LHPC Green:2012ej), $N_f{=}2{+}1{+}1$ TMF (ETMC Alexandrou:2013wka), $N_f{=}2{+}1{+}1$ HISQ (PNDME Bhattacharya:2015wna), $N_f{=}2$ TMF with Clover (ETMC Abdel-Rehim:2015owa).
  • Figure 4: Left: Lattice results for the isovector $\tilde{q}(x)$ using momenta $P_z$: $\frac{2\pi}{L}$ (red), $\frac{4\pi}{L}$ (green),$\frac{6\pi}{L}$ (cyan). Right: Unpolarized isovector $\tilde{q}(x)$ upon extrapolation in $P_z$ with 68$\%$ C.L (orange band). Brown (green) dotted line corresponds to global analysis of MSTW Martin:2009iq (CTEQ-JLab Owens:2012bv).
  • Figure 5: Left: Results for the isovector $\tilde{q}$ upon one-loop and mass corrections for the momentum $P_z=4\pi/4$ and for 0, 2 and 5 HYP smearing steps. Right: The quasi-distribution function $\tilde{q}$, the PDF without subtracting the mass correction $q$, and the final PDF, $q(0)$, shown for momentum $P_z=\frac{6\pi}{L}$. Various black lines show phenomenological results at 6.25 MeV$^2$ from MSTW Martin:2009iq (CJ12 Owens:2012bv), ABM11 Alekhin:2012ig.
  • ...and 6 more figures