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000860315 0247_ $$2ISSN$$a1550-2368
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000860315 0247_ $$2ISSN$$a2470-0010
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000860315 1001_ $$0P:(DE-Juel1)132090$$aEicker, N.$$b0$$ufzj
000860315 245__ $$aLight and strange hadron spectroscopy with dynamical Wilson fermions
000860315 260__ $$aMelville, NY$$bInst.812068$$c1998
000860315 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c1998-12-04
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000860315 520__ $$aWe present the final analysis of the light and strange hadron spectra from a full QCD lattice simulation with two degenerate dynamical sea quark flavors at β=5.6 on a 163×32 lattice. Four sets of sea quark masses corresponding to the range 0.69<~mπ/mρ<~0.83 are investigated. For reference we also ran a quenched simulation at βeff=6.0, which is the point of equal lattice spacing, a−1ρ. In the light sector, we find the chiral extrapolation to physical u and d masses to present a major source of uncertainty, comparable to the expected size of unquenching effects. From linear and quadratic fits we can estimate the errors in the hadron masses made from light quarks to be on a 15% level prior to the continuum extrapolation. For the hadrons with strange valence quark content, the NF=2 approximation to QCD appears not to cure the well-known failure of quenched QCD to reproduce the physical K−K* splitting.
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000860315 7001_ $$0P:(DE-HGF)0$$aLacock, P.$$b1
000860315 7001_ $$0P:(DE-HGF)0$$aSchilling, K.$$b2
000860315 7001_ $$0P:(DE-HGF)0$$aSpitz, A.$$b3
000860315 7001_ $$0P:(DE-HGF)0$$aGlässner, U.$$b4
000860315 7001_ $$0P:(DE-HGF)0$$aGüsken, S.$$b5
000860315 7001_ $$0P:(DE-HGF)0$$aHoeber, H.$$b6
000860315 7001_ $$0P:(DE-Juel1)132179$$aLippert, Th.$$b7$$ufzj
000860315 7001_ $$0P:(DE-HGF)0$$aStruckmann, Th.$$b8
000860315 7001_ $$0P:(DE-HGF)0$$aUeberholz, P.$$b9
000860315 7001_ $$0P:(DE-HGF)0$$aViehoff, J.$$b10
000860315 7001_ $$0P:(DE-HGF)0$$aRitzenhöfer, G.$$b11
000860315 77318 $$2Crossref$$3journal-article$$a10.1103/physrevd.59.014509$$b : American Physical Society (APS), 1998-12-04$$n1$$p014509$$tPhysical Review D$$v59$$x0556-2821$$y1998
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