The HAL QCD potential in I=1 π π system with the meson bound state
Abstract
In this paper, we investigate the HAL QCD potential in the I=1 π π scattering using the hybrid method for all-to-all propagators, in which a propagator is approximated by low-eigenmodes and the remaining high-eigenmode part is stochastically estimated. To verify the applicability of the hybrid method to systems containing quark creation/annihilation contributions such as the meson, we calculate the I=1 ππ potential with the 2+1 flavor gauge configurations on 163 × 32 lattice at the lattice spacing a ≈ 0.12 fm and (mπ,m) ≈ (870, 1230) MeV, in which the meson appears as a deeply-bound state. While we find that the naive stochastic evaluations for quark creation/annihilation contributions lead to extremely large statistical fluctuations, additional noise reduction methods enable us to obtain a sufficiently precise potential, which shows a strong attractive force. We also confirm that the binding energy and k3 δ obtained from our potential are roughly consistent with an existing meson bound state, within a large systematic error associated with our calculation, whose possible origin is also discussed.