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arXiv · hep-ph/9305204

Is Large Lepton Mixing Excluded?

Alexei Yu. Smirnov·David N. Spergel·John N. Bahcall
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Abstract

The original \bnum -(or $\barν_τ$-) energy spectrum from the gravitational collapse of a star has a larger average energy than the spectrum for \bnue since the opacity of \bnue exeeds that of \bnum (or $ν_τ$). Flavor neutrino conversion, \bnue $\leftrightarrow$ \bnum, induced by lepton mixing results in partial permutation of the original \bnue and \bnum spectra. An upper bound on the permutation factor, $p \leq 0.35$ (99$\%$ CL) is derived using the data from SN1987A and the different models of the neutrino burst. The relation between the permutation factor and the vacuum mixing angle is established, which leads to the upper bound on this angle. The excluded region, $\sin^2 2θ> 0.7 - 0.9$, covers the regions of large mixing angle solutions of the solar neutrino problem: ``just-so" and, partly, MSW, as well as part of region of $ν_{e} - ν_μ$ oscillation space which could be responsible for the atmospheric muon neutrino deficit. These limits are sensitive to the predicted neutrino spectrum and can be strengthened as supernova models improve.

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Alexei Yu. Smirnov, David N. Spergel, John N. Bahcall. 1993-06-02. Is Large Lepton Mixing Excluded?. https://doi.org/10.1103/physrevd.49.1389

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