Abstract
The stable chromomagnetic vacuum for SU(2) Yang–Mills theory found earlier is shown to give a model for confinement in QCD, using Wilson loop and a linear potential (in the leading order) for quark–antiquark interaction. The coefficient k in this potential is found to be ~ 0.25 GeV2, in satisfactory agreement with nonrelativistic potential model calculations for charmonium. At finite temperature, the real effective energy density found earlier is used to obtain estimates of the deconfining temperature agreeing reasonably with lattice study for SU(2).
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