QCD Laplace sum rules are used to calculate heavy quarkonium (charmonium and bottomonium) hybrid masses in several distinct J P C channels. Previous studies of heavy quarkonium hybrids did not include the effects of dimension-six condensates, leading to unstable sum rules and unreliable mass predictions in some channels. We have updated these sum rules to include dimension-six condensates, providing new mass predictions for the spectra of heavy quarkonium hybrids. We confirm the finding of other approaches that the negative-parity J P C = (0, 1, 2) −+ , 1 −− states form the lightest hybrid supermultiplet and the positive-parity J P C = (0, 1) +− , (0, 1, 2) ++ states are members of a heavier supermultiplet. Our results disfavor a pure charmonium hybrid interpretation of the X(3872), in agreement with previous work.