In this work, we systematically calculate the mass spectra of the S-wave fully heavy tetraquark states bbbb, cccc, and bbcc in two nonrelativistic quark models. A tetraquark state may be an admixture of a 6c −6c state and a3c − 3c one, where 6c −6c(3c − 3c) denotes the color configuration with a 6c (3c) diquark and a6c (3c) antidiquark. For the tetraquark states bbbb and cccc with J P C = 0 ++ , the 6c −6c state is lower than the3c − 3c one in both the two quark models, while the order of the bbcc states depend on models. The 6c −6c and3c − 3c mixing effects are induced by the hyperfine interactions between the diquark and antidiquark, while the contributions from the one-gluon-exchange (OGE) Coulomb or the linear confinement potentials vanish for the QQQ Q system. With the couple-channel effects, we obtain the similar mass spectra. The numerical results show that the ground QQQ Q (Q = b, c and Q = b, c) tetraquark states are located above the corresponding scattering states, which indicates that there may not exist a bound state in the scheme of the two quark models.