KM3NeT/ORCA6 measures tau-neutrino normalization S_tau = 0.48 (+0.5/-0.33), a tau-neutrino CC cross section of (2.5 +2.6/-1.8) x 10^-38 cm^2/nucleon at 20.3 GeV, and alpha33 > 0.95 at 95% CL.
Measuring tau neutrino appearance probability via unitarity
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abstract
We propose a {\em unitarity method} for determining $\tau$ neutrino appearance probability $P(\nu_{\mu} \rightarrow \nu_{\tau})$ in long-baseline (LBL) accelerator experiments and atmospheric neutrino observations. When simultaneous in situ measurements of $P(\nu_{\mu} \rightarrow \nu_{\mu})$ and $P(\nu_{\mu} \rightarrow \nu_{e})$ proceed, as is typical in the LBL experiments, one can use unitarity to "measure" $P(\nu_{\mu} \rightarrow \nu_{\tau})$. A theorists' toy analysis for the model-independent determination of $P(\nu_{\mu} \rightarrow \nu_{\mu})$ and $P(\nu_{\mu} \rightarrow \nu_{e})$ is presented by using the NOvA data. It is shown in our analysis that $\lsim$5\% (8\%) measurement of $\tau$ neutrino appearance probability in neutrino (antineutrino) mode is possible in the peak region $1.5 \lesssim E_\nu \lesssim 2.5$ GeV. The $\nu$SM-independent nature of determination of the probabilities is emphasized.
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Study of tau neutrinos and non-unitary neutrino mixing with the first six detection units of KM3NeT/ORCA
KM3NeT/ORCA6 measures tau-neutrino normalization S_tau = 0.48 (+0.5/-0.33), a tau-neutrino CC cross section of (2.5 +2.6/-1.8) x 10^-38 cm^2/nucleon at 20.3 GeV, and alpha33 > 0.95 at 95% CL.