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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 .

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