Quantum Chromodynamics with Many Flavors
arXiv:hep-lat/9804005 · doi:10.1143/PTPS.131.415
Abstract
We investigate the phase structure of lattice QCD for general number of flavors . Based on numerical data combined with the results of the perturbation theory we propose the following picture: When , there is only one IR fixed point at vanishing gauge coupling, i.e., the theory in the continuum limit is trivial. On the other hand, when , there is a non-trivial fixed point. Therefore, the theory is non-trivial with anomalous dimensions, however, without quark confinement. Theories which satisfy both quark confinement and spontaneous chiral symmetry breaking in the continuum limit exist only for .
Talk presented by K. Kanaya at the 1997 Yukawa International Seminar (YKIS'97) on ``Non-Perturbative QCD --- Structure of the QCD Vacuum ---'', YITP, Kyoto, Japan, 2--12 Dec. 1997. To be published in the proceedings [Prog. Theor. Phys. Suppl.]
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