We demonstrate that the Standard Model amplitude for f1fˉ2→W±Z at the Born-level exhibits an approximate zero located at
cosθ=(g−f1+g−f2)/(g−f1−g−f2) at
high energies, where the g−fi (i=1,2) are the left-handed couplings
of the Z-boson to fermions and θ is the center of mass scattering
angle of the W-boson. The approximate zero is the combined result of an exact
zero in the dominant helicity amplitudes M(±,∓) and strong gauge
cancelations in the remaining amplitudes. For non-standard WWZ couplings
these cancelations no longer occur and the approximate amplitude zero is
eliminated.Comment: 11 pages, 4 figures submitted separately as uuencoded tar-ed
postscript files, FSU-HEP-940307, UCD-94-