TY - JOUR

T1 - Nucleon axial charge in (2+1)-flavor dynamical-lattice QCD with domain-wall fermions

AU - Yamazaki, T.

AU - Aoki, Y.

AU - Blum, T.

AU - Lin, H. W.

AU - Lin, M. F.

AU - Ohta, S.

AU - Sasaki, S.

AU - Tweedie, R. J.

AU - Zanotti, J. M.

PY - 2008/4/28

Y1 - 2008/4/28

N2 - We present results for the nucleon axial charge gA at a fixed lattice spacing of 1/a=1.73(3)GeV using 2+1 flavors of domain wall fermions on size 163×32 and 243×64 lattices (L=1.8 and 2.7 fm) with length 16 in the fifth dimension. The length of the Monte Carlo trajectory at the lightest mπ is 7360 units, including 900 for thermalization. We find finite volume effects are larger than the pion mass dependence at mπ=330MeV. We also find a scaling with the single variable mπL which can also be seen in previous two-flavor domain wall and Wilson fermion calculations. Using this scaling to eliminate the finite-volume effect, we obtain gA=1.20(6)(4) at the physical pion mass, mπ=135MeV, where the first and second errors are statistical and systematic. The observed finite-volume scaling also appears in similar quenched simulations, but disappear when V (2.4fm)3. We argue this is a dynamical quark effect.

AB - We present results for the nucleon axial charge gA at a fixed lattice spacing of 1/a=1.73(3)GeV using 2+1 flavors of domain wall fermions on size 163×32 and 243×64 lattices (L=1.8 and 2.7 fm) with length 16 in the fifth dimension. The length of the Monte Carlo trajectory at the lightest mπ is 7360 units, including 900 for thermalization. We find finite volume effects are larger than the pion mass dependence at mπ=330MeV. We also find a scaling with the single variable mπL which can also be seen in previous two-flavor domain wall and Wilson fermion calculations. Using this scaling to eliminate the finite-volume effect, we obtain gA=1.20(6)(4) at the physical pion mass, mπ=135MeV, where the first and second errors are statistical and systematic. The observed finite-volume scaling also appears in similar quenched simulations, but disappear when V (2.4fm)3. We argue this is a dynamical quark effect.

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U2 - 10.1103/PhysRevLett.100.171602

DO - 10.1103/PhysRevLett.100.171602

M3 - Article

AN - SCOPUS:43049140504

VL - 100

JO - Physical Review Letters

JF - Physical Review Letters

SN - 0031-9007

IS - 17

M1 - 171602

ER -