Two-flavor lattice QCD simulation in the epsilon-regime with exact chiral symmetry
JLQCD collaboration: H. Fukaya, S. Aoki, T.W. Chiu, S. Hashimoto, T., Kaneko, H. Matsufuru, J. Noaki, K. Ogawa, M. Okamoto, T. Onogi, N. Yamada

TL;DR
This paper reports on lattice QCD simulations with exact chiral symmetry in the epsilon-regime, confirming theoretical predictions and extracting the chiral condensate with high precision.
Contribution
It demonstrates the feasibility of simulating two-flavor QCD with exact chiral symmetry in the epsilon-regime and validates the Dirac eigenvalue spectrum against chiral random matrix theory.
Findings
Dirac eigenvalue spectrum agrees with chiral random matrix theory
Chiral condensate measured as (251(7)(11) MeV)^3
Simulation achieved at light quark mass of 3 MeV
Abstract
We perform lattice simulations of two-flavor QCD using Neuberger's overlap fermion, with which the exact chiral symmetry is realized at finite lattice spacings. The epsilon-regime is reached by decreasing the light quark mass down to 3 MeV on a 16^3 32 lattice with a lattice spacing \sim 0.11 fm. We find a good agreement of the low-lying Dirac eigenvalue spectrum with the analytical predictions of the chiral random matrix theory, which reduces to the chiral perturbation theory in the epsilon-regime. The chiral condensate is extracted as \Sigma(2 GeV) = (251(7)(11) MeV)^3, where the errors are statistical and an estimate of the higher order effects in the epsilon-expansion.
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