Abstract

We demonstrate that the Standard Model amplitude for f1fˉ2W±Zf_1 \bar f_2 \rightarrow W^\pm Z at the Born-level exhibits an approximate zero located at cosθ=(gf1+gf2)/(gf1gf2)\cos\theta = (g^{f_1}_{-} + g^{f_2}_{-}) / (g^{f_1}_{-} - g^{f_2}_{-}) at high energies, where the gfig^{f_i}_{-} (i=1,2i=1,2) are the left-handed couplings of the ZZ-boson to fermions and θ\theta is the center of mass scattering angle of the WW-boson. The approximate zero is the combined result of an exact zero in the dominant helicity amplitudes M(±,){\cal M}(\pm,\mp) and strong gauge cancelations in the remaining amplitudes. For non-standard WWZWWZ 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-

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    Last time updated on 01/04/2019