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Impact of Dynamical Charm Quark and Mixed Action Effect on Light Hadron Masses and Decay Constants

Tong-Wei Lin, Zun-Xian Zhang, Mengchu Cai, Hai-Yang Du, Bolun Hu, Xiangyu Jiang, Xiao-Lan Meng, Ji-Hao Wang, Peng Sun, Yi-Bo Yang, Dian-Jun Zhao

Abstract

We investigate the impact of including a dynamical charm quark on the properties of light hadrons. Our study uses gauge ensembles generated with the tadpole-improved Symanzik gauge action, comparing 2+1+1 flavor (HISQ fermion) ensembles at four lattice spacings to 2+1 flavor (clover fermion) ensembles at six lattice spacings. For the light and strange flavor observables, we employ the same tadpole-improved clover fermion action. From numerical results for light and strange quark masses, pion and kaon decay constants, and $Ω$ baryon masses, we find that the values obtained after continuum, chiral, and infinite-volume extrapolations are consistent within uncertainties. Even though the mixed action setup can introduce additional discretization effects, our calculation shows evidences that those effects can cancel with the discretization error in the unitary setup, resulting in better convergence in the continuum extrapolation.

Impact of Dynamical Charm Quark and Mixed Action Effect on Light Hadron Masses and Decay Constants

Abstract

We investigate the impact of including a dynamical charm quark on the properties of light hadrons. Our study uses gauge ensembles generated with the tadpole-improved Symanzik gauge action, comparing 2+1+1 flavor (HISQ fermion) ensembles at four lattice spacings to 2+1 flavor (clover fermion) ensembles at six lattice spacings. For the light and strange flavor observables, we employ the same tadpole-improved clover fermion action. From numerical results for light and strange quark masses, pion and kaon decay constants, and baryon masses, we find that the values obtained after continuum, chiral, and infinite-volume extrapolations are consistent within uncertainties. Even though the mixed action setup can introduce additional discretization effects, our calculation shows evidences that those effects can cancel with the discretization error in the unitary setup, resulting in better convergence in the continuum extrapolation.
Paper Structure (4 sections, 11 equations, 5 figures, 6 tables)

This paper contains 4 sections, 11 equations, 5 figures, 6 tables.

Figures (5)

  • Figure 1: Lattice spacing dependence of the $m_{\phi}$ (upper panel) and $m_{\Omega}$ using the valence strange quark mass tuned to $m_{\eta_s}^{\mathrm{phys}}$ = 689.89(49) MeV .
  • Figure 2: Lattice spacing dependence of the charmonium masses $m_{\eta_c}$ and $m_{J/\psi}$ using the valence charm quark mass tuned to the physical $m_{D_s}$.
  • Figure 3: Lattice spacing dependence of the $f_{K}$ with the impacts from the unphysical strange and light quark masses corrected using the parameters obtained from the joint fit.
  • Figure 4: $a^2(\mu^{\rm RI})^2$ dependence of $Z_A/Z_V$ at different lattice spacing using the $N_f=2+1$ unitary clover setup (left panel) and the $N_f=2+1+1$ clover on HISQ setup (right panel).
  • Figure 5: Similar to Fig. but for $Z_S/Z_P$.