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FLAVOR-SINGLET g_A FROM LATTICE QCD

S. J. Dong, J. -F. Lagae, K. F. Liu

TL;DR

A lattice QCD calculation of the flavor-singlet axial coupling constant $g_A$ of the proton from the axial-vector current is carried out on a quenched $16^3 \times 24$ lattice.

Abstract

We report on a lattice QCD calculation of the flavor-singlet axial coupling constant $g_A$ of the proton from the axial-vector current. The simulation is carried out at $β= 6$ on a quenched $16^3 \times 24$ lattice. An extrapolation to the chiral limit shows that the connected insertion (valence and cloud parts) is $0.62 \pm 0.09$, which is close to $g_A^8$. The disconnected insertion (vacuum polarization from the sea quark) for the $u$ or $d$ quark is $- 0.12\pm 0.01 $ and the $s$ quark also contributes $-0.12\pm 0.01$. The total $g_A^1$ is thus $0.25 \pm 0.12$ which is in agreement with experiments. In addition, we find $g_A^3 = 1.20 \pm 0.11$, $g_A^8 = 0.61 \pm 0.13$ and $F_A/D_A = 0.60 \pm 0.02$, also in agreement with experiments.

FLAVOR-SINGLET g_A FROM LATTICE QCD

TL;DR

A lattice QCD calculation of the flavor-singlet axial coupling constant of the proton from the axial-vector current is carried out on a quenched lattice.

Abstract

We report on a lattice QCD calculation of the flavor-singlet axial coupling constant of the proton from the axial-vector current. The simulation is carried out at on a quenched lattice. An extrapolation to the chiral limit shows that the connected insertion (valence and cloud parts) is , which is close to . The disconnected insertion (vacuum polarization from the sea quark) for the or quark is and the quark also contributes . The total is thus which is in agreement with experiments. In addition, we find , and , also in agreement with experiments.

Paper Structure

This paper contains 5 equations, 1 table.