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When $N_c =2$ we find the expected we find Coulomb-like behavior at short distances, $\\sim 1/x$ as the distance $x \\rightarrow 0$. In the planar limit at $N_c = \\infty$ we find a weaker singularity, $\\sim 1/\\sqrt{x}$ as $x \\rightarrow 0$. In each case, at short distances the behavior of the correlation functions between two Polyakov loops, and the corresponding Wilson loop, are the same. 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