Well, my solid state textbook (Streetman's) defines the quasi-Fermi level for holes with the following statement:
E_i - F_p = k T \ln{\frac{p}{n_i}}
So, for the difference to be negative, the number of holes would have to be less than the intrinsic number of holes. In an n-type semiconductor, this is definitely possible, so I would say that yes, the quasi-Fermi level for holes can be above the intrinsic level.
For example, consider steady-state optical generation. As the optical generation rate approaches zero, the semiconductor behaves more and more like it is at equilibrium. In that case, p approaches p_0, the equilibrium value, and the above equation becomes equivalent to the relation for semiconductors at equilibrium. Hence, in this case, both the quasi-Fermi level for holes and electrons approach the equilibrium Fermi level, which for n-type material, is clearly above the intrinsic value.