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We compute analytically the diagonal quark number susceptibilities for a quark–gluon plasma at finite temperature and zero chemical potential, and compare with recent lattice results. The calculation uses the approximately self-consistent resummation of hard thermal and dense loops that we have developed previously. For temperatures between 1.5 to 5Tc, our results follow the same trend as the lattice data, but exceed them in magnitude by about 5–10%. We also compute the lowest order contribution, of order αs3log(1/αs), to the off-diagonal susceptibility. This contribution, which is not a part of our self-consistent calculation, is numerically small, but not small enough to be compatible with a recent lattice simulation.
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Blaizot et al. (2001) studied this question.
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