  The average density of states in a disordered three-dimensional Weyl system
is discussed in the case of a continuous distribution of random scattering. Our
result clearly indicate that the average density of states does not vanish,
reflecting the absence of a critical point for a metal-insulator transition.
This calculation supports recent suggestions of an avoided quantum critical
point in the disordered three-dimensional Weyl semimetal. However, the
effective density of states can be very small such that the
saddle-approximation with a vanishing density of states might be valid for
practical cases.
