Light hadron spectrum and quark masses from quenched lattice QCD

S. Aoki, G. Boyd, R. Burkhalter, S. Ejiri, M. Fukugita, S. Hashimoto, Y. Iwasaki, K. Kanaya, T. Kaneko, Y. Kuramashi, K. Nagai, M. Okawa, H. P. Shanahan, A. Ukawa, and T. Yoshié (CP-PACS Collaboration)
Phys. Rev. D 67, 034503 – Published 13 February 2003
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Abstract

We present the details of simulations for the light hadron spectrum in quenched QCD carried out on the CP-PACS parallel computer. Simulations are made with the Wilson quark action and the plaquette gauge action on lattices of size 323×56643×112 at four values of lattice spacings in the range a0.10.05fm and spatial extent Lsa3fm. Hadronic observables are calculated at five quark masses corresponding to mPS/mV0.750.4, assuming the u and d quarks are degenerate, but treating the s quark separately. We find that the presence of quenched chiral singularities is supported from an analysis of the pseudoscalar meson data. The physical values of hadron masses are determined using mπ, mρ, and mK (or mφ) as input to fix the physical scale of lattice spacing and the u, d, and s quark masses. After chiral and continuum extrapolations, the agreement of the calculated mass spectrum with experiment is at a 10% level. In comparison with the statistical accuracy of 1%–3% and systematic errors of at most 1.7% we have achieved, this demonstrates a failure of the quenched approximation for the hadron spectrum: the hyperfine splitting in the meson sector is too small, and in the baryon sector the octet masses and mass splitting of the decuplet are both smaller than experiment. Light quark masses are calculated using two definitions: the conventional one and the one based on the axial-vector Ward identity. The two results converge toward the continuum limit, yielding mud=4.29(14)0.79+0.51MeV where the first error is statistical and the second one is systematic due to chiral extrapolation. The s quark mass depends on the strange hadron mass chosen for input: ms=113.8(2.3)2.9+5.8MeV from mK and ms=142.3(5.8)0+22.0MeV from mφ, indicating again a failure of the quenched approximation. We obtain the scale of QCD, ΛMS¯(0)=219.5(5.4)MeV with mρ used as input. An O(10%) deviation from experiment is observed in the pseudoscalar meson decay constants.

  • Received 17 June 2002

DOI:https://doi.org/10.1103/PhysRevD.67.034503

©2003 American Physical Society

Authors & Affiliations

S. Aoki1, G. Boyd2,*, R. Burkhalter1,2,†, S. Ejiri2,‡, M. Fukugita3, S. Hashimoto4, Y. Iwasaki1,2, K. Kanaya1,2, T. Kaneko2,§, Y. Kuramashi4, K. Nagai2,∥, M. Okawa4,¶, H. P. Shanahan2,**, A. Ukawa1,2, and T. Yoshié1,2

  • 1Institute of Physics, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan
  • 2Center for Computational Physics, University of Tsukuba, Tsukuba, Ibaraki 305-8577, Japan
  • 3Institute for Cosmic Ray Research, University of Tokyo, Tanashi, Tokyo 188-8502, Japan
  • 4High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan

  • *Present address: Packaging and Device Development, Procter and Gamble, Temselaan 100, B-1853 Strombeek-Bever, Belgium.
  • Present address: KPMG Consulting AG, Badenerstrasse 172, 8804 Zurich, Switzerland.
  • Present address: Department of Physics, University of Wales, Swansea SA2 8PP, UK.
  • §Present address: High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan.
  • Present address: CERN, Theory Division, CH-1211 Geneva 23, Switzerland.
  • Present address: Department of Physics, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8526, Japan.
  • **Present address: European Bioinformatics Institute, Wellcome Trust Genome Campus, Hinxton, Cambridge, CB10 1SD, UK.

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Vol. 67, Iss. 3 — 1 February 2003

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