We consider the interpretation of the MiniBooNE low-energy anomaly and the gallium radioactive source experiments anomaly in terms of short-baseline electron neutrino disappearance in the framework of 3 + 1 four-neutrino mixing schemes. The separate fits of MiniBooNE and gallium data are highly compatible, with close best-fit values of the effective oscillation parameters Delta m(2) and sin(2)upsilon. The combined fit gives Delta m(2) greater than or similar to 0.1 eV(2) and 0.11 less than or similar to sin(2)2 upsilon less than or similar to 0.48 at 2 sigma. We consider also the data of the Bugey and Chooz reactor antineutrino oscillation experiments and the limits on the effective electron antineutrino mass in beta decay obtained in the Mainz and Troitsk tritium experiments. The fit of the data of these experiments limits the value of sin(2)2 upsilon below 0.10 at 2 sigma. Considering the tension between the neutrino MiniBooNE and gallium data and the antineutrino reactor and tritium data as a statistical fluctuation, we perform a combined fit which gives Delta m(2) similar or equal to 2 eV and 0.01 less than or similar to sin(2)2 upsilon less than or similar to 0.13 at 2 sigma. Assuming a hierarchy of masses m1, m2, m3 << m4, the predicted contributions of m4 to the effective neutrino masses in beta decay and neutrinoless double-beta decay are, respectively, between about 0.06 and 0.49 and between about 0.003 and 0.07 eV at 2 sigma. We also consider the possibility of reconciling the tension between the neutrino MiniBooNE and gallium data and the antineutrino reactor and tritium data with different mixings in the neutrino and antineutrino sectors. We find a 2.6 sigma indication of a mixing angle asymmetry.
Short-baseline electron neutrino disappearance, tritium beta decay, and neutrinoless double-beta decay
LAVEDER, MARCO
2010
Abstract
We consider the interpretation of the MiniBooNE low-energy anomaly and the gallium radioactive source experiments anomaly in terms of short-baseline electron neutrino disappearance in the framework of 3 + 1 four-neutrino mixing schemes. The separate fits of MiniBooNE and gallium data are highly compatible, with close best-fit values of the effective oscillation parameters Delta m(2) and sin(2)upsilon. The combined fit gives Delta m(2) greater than or similar to 0.1 eV(2) and 0.11 less than or similar to sin(2)2 upsilon less than or similar to 0.48 at 2 sigma. We consider also the data of the Bugey and Chooz reactor antineutrino oscillation experiments and the limits on the effective electron antineutrino mass in beta decay obtained in the Mainz and Troitsk tritium experiments. The fit of the data of these experiments limits the value of sin(2)2 upsilon below 0.10 at 2 sigma. Considering the tension between the neutrino MiniBooNE and gallium data and the antineutrino reactor and tritium data as a statistical fluctuation, we perform a combined fit which gives Delta m(2) similar or equal to 2 eV and 0.01 less than or similar to sin(2)2 upsilon less than or similar to 0.13 at 2 sigma. Assuming a hierarchy of masses m1, m2, m3 << m4, the predicted contributions of m4 to the effective neutrino masses in beta decay and neutrinoless double-beta decay are, respectively, between about 0.06 and 0.49 and between about 0.003 and 0.07 eV at 2 sigma. We also consider the possibility of reconciling the tension between the neutrino MiniBooNE and gallium data and the antineutrino reactor and tritium data with different mixings in the neutrino and antineutrino sectors. We find a 2.6 sigma indication of a mixing angle asymmetry.Pubblicazioni consigliate
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