Neutrino-antineutrino interchange of chiral scattering weights

Crossing a massless neutrino to an antineutrino reverses the antisymmetric part of its spin tensor. The $s^2$ and $u^2$ weights exchange, giving ${\sigma }_{\bar{\nu }}=G_F^{2}s[(c_V-c_A{)}^2+(c_V+c_A{)}^2/3]/(4\pi )$ for the same electron couplings. This is a low-energy contact statement rather than a replacement for a full weak-boson propagator.