Abstract

A simple model is presented that describes the free energy W(J)W(J) of QCD coupled to an external current that is a single plane wave, J(x)=Hcos⁡(k⋅x)J(x) = H \cos(k \cdot x). The model satisfies a bound obtained previously on W(J)W(J) that comes from the Gribov horizon. If one uses this model to fit recent lattice data --- which give for the gluon propagator D(k)D(k) a non-zero value, D(0)≠0D(0) \neq 0, at k=0k = 0 --- the data favor a non-analyticity in W(J)W(J).

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