Determination of the chiral condensate from 2+1-flavor lattice QCD
The JLQCD collaboration: H. Fukaya, S. Aoki, S. Hashimoto, T. Kaneko,, J. Noaki, T. Onogi, N. Yamada

TL;DR
This paper presents a precise lattice QCD calculation of the 2+1-flavor chiral condensate using overlap quarks, matching eigenvalue spectra with chiral perturbation theory to achieve accurate results.
Contribution
It introduces a novel method of determining the chiral condensate by combining lattice QCD with eigenvalue spectrum analysis in the epsilon-regime.
Findings
Chiral condensate value: 242(4)(+19-18) MeV^3 at 2 GeV
Successful matching of eigenvalue spectrum with chiral perturbation theory
Precise determination of the condensate with controlled errors
Abstract
We perform a precise calculation of the chiral condensate in QCD using lattice QCD with 2+1 flavors of dynamical overlap quarks. Up and down quark masses cover a range between 3 and 100 MeV on a 16^3x48 lattice at a lattice spacing around 0.11 fm. At the lightest sea quark mass, the finite volume system on the lattice is in the epsilon-regime. By matching the low-lying eigenvalue spectrum of the Dirac operator with the prediction of chiral perturbation theory at the next-to-leading order, we determine the chiral condensate in 2+1-flavor QCD with strange quark mass fixed at its physical value as Sigma (MS-bar at 2 GeV) = [242(04)(^+19_-18}) MeV}]^3, where the errors are statistical and systematic, respectively.
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