The conceptual difficulties affecting the definition of the neutrino electromagnetic form factor are briefly reviewed in the context of the standard model. It is then shown that the radiative corrections Δ^(ν;l)(q²) and Δ^(ν;h)(q²) relevant to {ν}-lepton and {ν}-hadron scattering in the renormalization scheme in which sin²{{{θ}}}W≡1-{m}W²$/${m}Z²$, can be separated into two finite and gauge-invariant parts. One part ${{Δ}}^{({ν})}$(${q}²$) is target independent and the associated function f(${q}²)≡-{q}²Δ^(ν) (q²)/(2mW²) can be interpreted as an effective electromagnetic form factor of the neutrino in the framework of the low-energy theory derived from the standard model at invariant mass scales {}mW². The observability of this quantity and its dependence on the top-quark mass and the neutrino flavor are discussed. Updated estimates of the hadronic contributions to Δ^(ν)(q²) are given. A strategy to search for {ν} structure beyond the standard model is outlined.
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Degrassi et al. (1989) studied this question.
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