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There is no reason you can't have nuclear or nucleon excitation; or meson production reactions in the mix. Reaction like $$ \nu + ^{16}\!\mathrm{O} \to \nu + ^{16}\!\mathrm{O}^* \,$$ with a subsequent decay of the excited nucleus or $$ \nu + n \to e^- + \Delta^+ \,,$$ or $$ \nu + p \to e^- + p + \pi^+ \,,$$ are accessible. The three I have exhibited will ...


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The thing is that any reaction which produces a charged particle traveling faster than local $c$ will produce Cherenkov radiation. In a neutrino experiment the two you list are the signal, and any others are the background. Someone else analyzing the same data from the same detector might not be interested in the neutrino signal and consider that ...


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The only neutrino interactions known to be detected are those you provided: The charged current interaction and the neutral current interaction, respectively. These interactions can also be differentiated with respect to flavor. In IceCube, for example, the charged-current interaction from a muon neutrino produces a "track" in the detector along the path of ...



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