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$η$ and $η'$ mesons from $N_f = 2+1$ lattice QCD at the physical point using topological charge operators

Yue Su, Nan Wang, Long-cheng Gui, Jun Hua, Jian Liang, Jun Shi

TL;DR

This work addresses the challenge of determining η and η' masses and their SU(3) flavor mixing in lattice QCD by using topological charge density operators on two 2+1-flavor ensembles at the physical point. The authors compute 4D topological-charge correlators, apply Wilson-flow smearing, and fit the resulting spectra with large-$\hat{r}$ single-state and constrained two-state forms to extract $m_\eta$, $m_{\eta'}$, and $\theta_1$, arriving at $m_\eta = 0.505(72)(75)$ GeV, $m_{\eta'} = 0.952(47)(40)$ GeV, and $\theta_1 = -8.9(2.1)(1.8)^{\circ}$. The analysis demonstrates that topological charge operators can effectively probe flavor-singlet mesons, offering a cross-check against quark-bilinear methods and a path toward higher-precision results with more configurations. The study also provides insight into the interplay between topology, the U_A(1) anomaly, and η–η' mixing in QCD.

Abstract

By fitting the two-point correlation functions of topological charge density operators calculated on two $2+1$-flavor gauge ensembles with physical pion mass, we determine both the $η$ and $η'$ masses and also the mixing angle to be $m_η= 0.505(72)(75)$ GeV, $m_{η'}=0.952(47)(40)$ GeV, and $θ_1 = -8.9(2.1)(1.8)^\circ$, respectively, where the first error is the statistical uncertainty and the second one is the systematic uncertainty. This is the first extraction of both $η/η'$ masses and the mixing angle $θ_1$ using topological charge operators. Compared with previous studies using quark bilinear operators, the error of the $η$ mass is relatively large, but the mixing angle has comparable precision. This demonstrates that the topological charge operators are well suited to study the $η$ and $η'$ mesons.

$η$ and $η'$ mesons from $N_f = 2+1$ lattice QCD at the physical point using topological charge operators

TL;DR

This work addresses the challenge of determining η and η' masses and their SU(3) flavor mixing in lattice QCD by using topological charge density operators on two 2+1-flavor ensembles at the physical point. The authors compute 4D topological-charge correlators, apply Wilson-flow smearing, and fit the resulting spectra with large- single-state and constrained two-state forms to extract , , and , arriving at GeV, GeV, and . The analysis demonstrates that topological charge operators can effectively probe flavor-singlet mesons, offering a cross-check against quark-bilinear methods and a path toward higher-precision results with more configurations. The study also provides insight into the interplay between topology, the U_A(1) anomaly, and η–η' mixing in QCD.

Abstract

By fitting the two-point correlation functions of topological charge density operators calculated on two -flavor gauge ensembles with physical pion mass, we determine both the and masses and also the mixing angle to be GeV, GeV, and , respectively, where the first error is the statistical uncertainty and the second one is the systematic uncertainty. This is the first extraction of both masses and the mixing angle using topological charge operators. Compared with previous studies using quark bilinear operators, the error of the mass is relatively large, but the mixing angle has comparable precision. This demonstrates that the topological charge operators are well suited to study the and mesons.

Paper Structure

This paper contains 7 sections, 10 equations, 8 figures, 1 table.

Figures (8)

  • Figure 1: The two-point correlation function of the topological charge density operator $C_2(r)$ as a function of $r$ on the 48I ensemble. The zoomed in figure shows the negative correlation at large $r$.
  • Figure 2: The correlation functions of topological charge density operators on the 64I ensembles. Additional minus sign is included and the data points with different flow times are shifted vertically for clarity.
  • Figure 3: The topological charges of several different gauge configurations as a function of flow time on the 64I lattice. The horizontal dashed lines indicate the nearest integers.
  • Figure 4: The effective masses and fitting results of the $\eta$ mass. The bands also indicate the fitting ranges.
  • Figure 5: Left panel: single-state fitting results for the $\eta$ mass on the 64I ensemble as a function of the fitting starting point $\hat{r}_{\rm start}$. The corresponding $\chi^2/\text{d.o.f.}$ are also presented. The bands are to indicate the picked fitting and to show more clearly the difference of the fitting results between different $\hat{r}_{\rm start}$. Right panel: the same plot but for the 48I ensemble.
  • ...and 3 more figures