Abstract:Neutrino-antineutrino conversion is an important new physics process. The observation of this phenomenon could indicate total lepton number violation and potential CPT-violation. Searching for the appearance of electron antineutrinos from solar neutrinos from 8 B decay allows us to hunt for this rare process, although it can also be explained by other mechanisms or hypotheses. This analysis examines the capabilities of observing neutrino-antineutrino transition from 8 B unoscillated solar neutrinos using diffe… Show more
“…The increased detection efficiencies at lower energies, and reduced accidental and mis-reconstructed backgrounds will improve on the limits we set, being limited only by intrinsic reactor and atmospheric ν e backgrounds. Future large liquid-scintillator detectors, such as the Jiangmen Underground Neutrino Observatory (JUNO) [64] and the Jinping neutrino experiment [65], can also improve on current constraints with an expected threshold of E ν 8.5 MeV [66]. In the far future, observatories capable of accumulating larger numbers of DSNB events, such as the proposed detector THEIA [67], would play an important role in searching for solar antineutrinos.…”
Solar neutrino experiments are highly sensitive to sources of ν → ν conversions in the 8 B neutrino flux. In this work we adapt these searches to non-minimal sterile neutrino models recently proposed to explain the LSND, MiniBooNE, and reactor anomalies. The production of such sterile neutrinos in the Sun, followed the decay chain ν4 → νϕ → ννν with a new scalar ϕ results in upper limits for the neutrino mixing |Ue4| 2 at the per mille level. We conclude that a simultaneous explanations of all anomalies is in tension with KamLAND, Super-Kamiokande, and Borexino constraints on the flux of solar antineutrinos. We then present other minimal models that violate parity or lepton number, and discuss the applicability of our constraints in each case. Future improvements can be expected from existing Borexino data as well as from future searches at Super-Kamiokande with added Gd.
“…The increased detection efficiencies at lower energies, and reduced accidental and mis-reconstructed backgrounds will improve on the limits we set, being limited only by intrinsic reactor and atmospheric ν e backgrounds. Future large liquid-scintillator detectors, such as the Jiangmen Underground Neutrino Observatory (JUNO) [64] and the Jinping neutrino experiment [65], can also improve on current constraints with an expected threshold of E ν 8.5 MeV [66]. In the far future, observatories capable of accumulating larger numbers of DSNB events, such as the proposed detector THEIA [67], would play an important role in searching for solar antineutrinos.…”
Solar neutrino experiments are highly sensitive to sources of ν → ν conversions in the 8 B neutrino flux. In this work we adapt these searches to non-minimal sterile neutrino models recently proposed to explain the LSND, MiniBooNE, and reactor anomalies. The production of such sterile neutrinos in the Sun, followed the decay chain ν4 → νϕ → ννν with a new scalar ϕ results in upper limits for the neutrino mixing |Ue4| 2 at the per mille level. We conclude that a simultaneous explanations of all anomalies is in tension with KamLAND, Super-Kamiokande, and Borexino constraints on the flux of solar antineutrinos. We then present other minimal models that violate parity or lepton number, and discuss the applicability of our constraints in each case. Future improvements can be expected from existing Borexino data as well as from future searches at Super-Kamiokande with added Gd.
“…The solar metallicity problem [11,12] will profit from either precise measurements of the Be and B solar neutrino fluxes, or the observation of solar neutrinos from the CNO cycle. On the elementary particle side, validation tests of the large mix- ing angle (LMA) Mikheyev-Smirnov-Wolfenstein (MSW) [13,14] solution and the search for new physics beyond the standard scenario [15][16][17][18] constitute the main goals. The standard scenario of three neutrino mixing predicts a smooth upturn in the survival probability ( ) in the neutrino energy region between the high (MSW dominated) and low (vacuum dominated) ranges, and a sizable Day-Night asymmetry at the percentage level.…”
The Jiangmen Underground Neutrino Observatory (JUNO) features a 20 kt multi-purpose underground liquid scintillator sphere as its main detector. Some of JUNO's features make it an excellent location for
B solar neutrino measurements, such as its low-energy threshold, high energy resolution compared with water Cherenkov detectors, and much larger target mass compared with previous liquid scintillator detectors. In this paper, we present a comprehensive assessment of JUNO's potential for detecting
B solar neutrinos via the neutrino-electron elastic scattering process. A reduced 2 MeV threshold for the recoil electron energy is found to be achievable, assuming that the intrinsic radioactive background
U and
Th in the liquid scintillator can be controlled to 10
g/g. With ten years of data acquisition, approximately 60,000 signal and 30,000 background events are expected. This large sample will enable an examination of the distortion of the recoil electron spectrum that is dominated by the neutrino flavor transformation in the dense solar matter, which will shed new light on the inconsistency between the measured electron spectra and the predictions of the standard three-flavor neutrino oscillation framework. If
eV
, JUNO can provide evidence of neutrino oscillation in the Earth at approximately the 3
(2
) level by measuring the non-zero signal rate variation with respect to the solar zenith angle. Moreover, JUNO can simultaneously measure
using
B solar neutrinos to a precision of 20% or better, depending on the central value, and to sub-percent precision using reactor antineutrinos. A comparison of these two measurements from the same detector will help understand the current mild inconsistency between the value of
reported by solar neutrino experiments and the KamLAND experiment.
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