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We study the gluon propagator and the singlet potential in Landau gauge in the deconfined phase of SU(2) lattice gauge theory, using both the standard Wilson action and a tree-level Symanzik improved action. From the long-distance behavior of correlation functions of temporal and spatial components of the gauge fields we extract electric (mₑ) and magnetic (mₘ) screening masses. For the magnetic mass we find mₘ(T)=0.456(6)g²(T)T. The electric mass can be described by a next-to leading order ansatz, obtained from one loop resummed perturbation theory. However, the best description is given by mₑ(T)=√1.70(2)g(T)T. The electric screening mass thus is different from its lowest order perturbative prediction even for temperatures as high as T~10⁴Tc.
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Heller et al. (1998) studied this question.
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