Anomaly cancelation has been shown to occur in time-reversal symmetry-broken
Weyl metals, which explains the existence of a Fermi arc. We extend this result
in the case of inversion symmetry-broken Weyl metals. Constructing a minimal
model that takes a double pair of Weyl points, we demonstrate the anomaly
cancelation explicitly. This demonstration explains why a chiral pair of Fermi
arcs appear in inversion symmetry-broken Weyl metals. In particular, we find
that this pair of Fermi arcs gives rise to either "quantized" spin Hall or
valley Hall effects, which corresponds to the "quantized" version of the charge
Hall effect in time-reversal symmetry-broken Weyl metals