Two-flavor lattice QCD simulation in the epsilon-regime with exact chiral symmetry
| dc.creator | JLQCD collaboration | |
| dc.creator | Fukaya, H. | |
| dc.creator | Aoki, S. | |
| dc.creator | Chiu, T. W. | |
| dc.creator | Hashimoto, S. | |
| dc.creator | Kaneko, T. | |
| dc.creator | Matsufuru, H. | |
| dc.creator | Noaki, J. | |
| dc.creator | Ogawa, K. | |
| dc.creator | Okamoto, M. | |
| dc.creator | Onogi, T. | |
| dc.creator | Yamada, N. | |
| dc.date | 2007-02-02 | |
| dc.date.accessioned | 2026-07-07T11:01:58Z | |
| dc.date.available | 2026-07-07T11:01:58Z | |
| dc.description | 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 Σ(2 GeV) = (251(7)(11) MeV)^3, where the errors are statistical and an estimate of the higher order effects in the epsilon-expansion. | |
| dc.description | 10pages, 4figures | |
| dc.identifier | https://arxiv.org/abs/hep-lat/0702003 | |
| dc.identifier | http://arxiv.org/abs/hep-lat/0702003 | |
| dc.identifier | Phys.Rev.Lett.98:172001,2007 | |
| dc.identifier | doi:10.1103/PhysRevLett.98.172001 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/188109 | |
| dc.subject | High Energy Physics - Lattice | |
| dc.title | Two-flavor lattice QCD simulation in the epsilon-regime with exact chiral symmetry | |
| dc.type | text |