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Selected results on hadron structure using state-of-the-art lattice QCD simulations

Constantia Alexandrou

TL;DR

The paper surveys lattice QCD studies of hadron structure using simulations at near-physical parameters. It outlines a program computing hadron masses, the nucleon axial charge $g_A$, gluon and quark unpolarized moments including $\langle x \rangle$ and $\langle x \rangle_g$, and generalized parton distributions via twist-two operators such as $O_V^a$, $O_A^a$, and $O_T^a$, with $A_{20}$, $B_{20}$, and $C_{20}$ form factors. It reports that at the physical point $g_A$ agrees with experiment, quantifies SU(3) breaking with $\delta_{\rm SU(3)} \approx 0.10$--$0.15$ for octet baryons, and presents a spin decomposition $J^q=\tfrac{1}{2}[A_{20}^q(0)+B_{20}^q(0)]$ including disconnected contributions; it also explores direct quasi-PDF approaches and the associated renormalization/matching challenges. It demonstrates lattice QCD's reliability for hadron structure and points to rapid progress toward PDFs and ab initio nuclear physics as systematics are controlled ($a$, $L$, excited-state effects, and renormalization).

Abstract

We review progress on hadron structure using lattice QCD simulations at or near to physical values of the QCD parameters. In particular, we discuss recent results on hadron masses, the nucleon charges, spin, gluon and quark unpolarized moments, the axial charge of hyperons, and the pion unpolarized moment.

Selected results on hadron structure using state-of-the-art lattice QCD simulations

TL;DR

The paper surveys lattice QCD studies of hadron structure using simulations at near-physical parameters. It outlines a program computing hadron masses, the nucleon axial charge , gluon and quark unpolarized moments including and , and generalized parton distributions via twist-two operators such as , , and , with , , and form factors. It reports that at the physical point agrees with experiment, quantifies SU(3) breaking with -- for octet baryons, and presents a spin decomposition including disconnected contributions; it also explores direct quasi-PDF approaches and the associated renormalization/matching challenges. It demonstrates lattice QCD's reliability for hadron structure and points to rapid progress toward PDFs and ab initio nuclear physics as systematics are controlled (, , excited-state effects, and renormalization).

Abstract

We review progress on hadron structure using lattice QCD simulations at or near to physical values of the QCD parameters. In particular, we discuss recent results on hadron masses, the nucleon charges, spin, gluon and quark unpolarized moments, the axial charge of hyperons, and the pion unpolarized moment.

Paper Structure

This paper contains 6 sections, 5 equations, 8 figures.

Figures (8)

  • Figure 1: A summary of recent simulations showing the value of the pion mass and the lattice spacing: Black filled circles are from PACS using $N_f=2+1$ clover-improved fermions Aoki:2009ixIshikawa:2015rho, light blue filled circles from BMW for $N_f=2+1$ clover-improved fermions with HEX smearing Durr:2010aw, yellow filled diamonds from MILC using $N_f=2+1+1$ staggered fermions Bazavov:2012xda, magenta open circles from QCDSF using $N_f=2$ clover-improved fermions Horsley:2013ayv, green filled circles from CLS using $N_f=2+1$ clover-improved fermions Bruno:2014jqa, blue filled squares from RBC-UKQCD using domain wall fermions Boyle:2015hfa, red filled (open) circles from ETMC using $N_f=2+1+1$ twisted mass fermions ($N_f=2$ with a clover term) Abdel-Rehim:2015pwa. The size of the symbols is according to the value of $m_\pi L$ with the smallest value taken as $m_\pi L\sim 3$ and the largest $m_\pi L\sim 6.7$.
  • Figure 2: Left: The nucleon mass versus $a^2$ for $N_f=2$ twisted mass fermions (TMF) for various pion masses in units of $r_0=0.44$ fm (ETMC) Alexandrou:2008tn. Right top: Volume dependence of the nucleon mass for $m_\pi\sim 450$ MeV, $N_f=2+1$ Clover and $a\sim 0.12$ fm (NPLQCD) Orginos:2015aya. Right bottom: Effective masses of baryons using $N_f=2$ twisted mass clover-improved fermions at physical pion mass Alexandrou:2014wca.
  • Figure 3: Lattice QCD results on the nucleon $g_A$.
  • Figure 4: Left panel: The nucleon isovector tensor charge. Right panel: The isovector scalar charge.
  • Figure 5: The SU(3) breaking parameter $\delta_{\rm SU(3)}$ for the octet (left) and the decuplet (right). Results are from Refs. Lin:2007apAlexandrou:2014wca.
  • ...and 3 more figures