Masses and decay constants of the η and η′ mesons from lattice QCD

被引:48
作者
Bali, Gunnar S. [1 ,2 ]
Braun, Vladimir [1 ]
Collins, Sara [1 ]
Schaefer, Andreas [1 ]
Simeth, Jakob [1 ]
机构
[1] Univ Regensburg, Inst Theoret Phys, D-93040 Regensburg, Germany
[2] Tata Inst Fundamental Res, Homi Bhabha Rd, Mumbai 400005, Maharashtra, India
关键词
Lattice QCD; Chiral Lagrangians; 1/N Expansion; Anomalies in Field and String Theories; LARGE-N-C; DYNAMICS; MATRIX; RUNDEC; ORDER; LIMIT;
D O I
10.1007/JHEP08(2021)137
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
We determine the masses, the singlet and octet decay constants as well as the anomalous matrix elements of the eta and eta ' mesons in N-f = 2 + 1 QCD. The results are obtained using twenty-one CLS ensembles of non-perturbatively improved Wilson fermions that span four lattice spacings ranging from a approximate to 0.086 fm down to a approximate to 0.050 fm. The pion masses vary from M-pi = 420 MeV to 126 MeV and the spatial lattice extents L-s are such that LsM pi greater than or similar to 4, avoiding significant finite volume effects. The quark mass dependence of the data is tightly constrained by employing two trajectories in the quark mass plane, enabling a thorough investigation of U(3) large-N-c chiral perturbation theory (ChPT). The continuum limit extrapolated data turn out to be reasonably well described by the next-to-leading order ChPT parametrization and the respective low energy constants are determined. The data are shown to be consistent with the singlet axial Ward identity and, for the first time, also the matrix elements with the topological charge density are computed. We also derive the corresponding next-to-leading order large-N-c ChPT formulae. We find F-8 = 115.0(2.8) MeV, theta(8) = -25.8(2.3)degrees, theta(0) = -8.1(1.8)degrees and, in the (MS) over bar scheme for N-f = 3, F-0(mu = 2 GeV) = 100.1(3.0) MeV, where the decay constants read F-eta(8) = F-8 cos theta(8), F-eta '(8) = F-8 sin theta(8), F-eta(0) = -F-0 sin theta(0) and F-eta '(0) = F-0 cos theta(0). For the gluonic matrix elements, we obtain a(eta)(mu = 2 GeV) = 0.0170(10) GeV3 and a(eta ')(mu = 2 GeV) = 0.0381(84) GeV3, where statistical and all systematic errors are added in quadrature.
引用
收藏
页数:94
相关论文
共 132 条
[51]  
Del Debbio L, 2004, J HIGH ENERGY PHYS
[52]   Topological susceptibility and η′ meson mass from Nf=2 lattice QCD at the physical point [J].
Dimopoulos, P. ;
Helmes, C. ;
Jost, C. ;
Knippschild, B. ;
Kostrzewa, B. ;
Liu, L. ;
Ottnad, K. ;
Petschlies, M. ;
Urbach, C. ;
Wenger, U. ;
Werner, M. .
PHYSICAL REVIEW D, 2019, 99 (03)
[53]  
Ding M., PHYS REV D, V99
[54]   LARGE N, CHIRAL APPROACH TO PSEUDOSCALAR MASSES, MIXINGS AND DECAYS [J].
DIVECCHIA, P ;
NICODEMI, F ;
PETTORINO, R ;
VENEZIANO, G .
NUCLEAR PHYSICS B, 1981, 181 (02) :318-334
[55]   CHIRAL DYNAMICS IN THE LARGE N LIMIT [J].
DIVECCHIA, P ;
VENEZIANO, G .
NUCLEAR PHYSICS B, 1980, 171 (03) :253-272
[56]   Isoscalar meson spectroscopy from lattice QCD [J].
Dudek, Jozef J. ;
Edwards, Robert G. ;
Joo, Balint ;
Peardon, Michael J. ;
Richards, David G. ;
Thomas, Christopher E. .
PHYSICAL REVIEW D, 2011, 83 (11)
[57]  
Escribano R, 2005, J HIGH ENERGY PHYS, DOI 10.1088/1126-6708/2005/06/029
[58]   η′ transition form factor from space- and timelike experimental data [J].
Escribano, R. ;
Gonzalez-Solis, S. ;
Masjuan, P. ;
Sanchez-Puertas, P. .
PHYSICAL REVIEW D, 2016, 94 (05)
[59]  
Escribano R, 2015, EUR PHYS J C, V75, DOI 10.1140/epjc/s10052-015-3642-z
[60]   η and η′ transition form factors from rational approximants [J].
Escribano, Rafel ;
Masjuan, Pere ;
Sanchez-Puertas, Pablo .
PHYSICAL REVIEW D, 2014, 89 (03)