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Direct Measurements of Neutrino Mass
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The turn of the 21st century witnessed a sudden shift in our fundamental understanding of particle physics. While the minimal Standard Model predicts that neutrino masses are exactly zero, the discovery of neutrino oscillations proved the Standard Model wrong. Neutrino oscillation measurements, however, do not shed light on the scale of neutrino masses, nor the mechanism by which those are generated. The neutrino mass scale is most directly accessed by studying the energy spectrum generated by beta decay or electron capture -- a technique dating back to Enrico Fermi's formulation of radioactive decay. In this Article, we review the methods and techniques -- both past and present -- aimed at measuring neutrino masses kinematically. We focus on recent experimental developments that have emerged in the past decade, overview the spectral refinements that are essential in the treatment of the most sensitive experiments, and give a simple yet effective protocol for estimating the sensitivity. Finally, we provide an outlook of what future experiments might be able to achieve.
Forward citations
Cited by 4 Pith papers
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Bound-state beta decay of tritium: Path to first observation and novel approach to direct neutrino mass measurement
Tritium bound-state beta decay could be seen in 3He de-excitation photons, and neutrino mass read from Doppler broadening of those emission lines.
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The real-time data processing and acquisition system for Project 8 Phase II
An FPGA plus software frequency-mask trigger records CRES events with 96.7% data reduction and under 0.5% efficiency variation for the Project 8 Phase II neutrino mass experiment.
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Another relation among the neutrino mass-squared differences?
The ratio (√Δm²31 + √Δm²21)/(√Δm²31 − √Δm²21) is claimed to be exactly √2, implying m1 ≈ 0 and absolute neutrino masses near 0.009 eV and 0.050 eV.
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Integral representation of the neutrino mass-squared differences
The claimed m1 < 0.0023 eV bound is an artifact of assuming the trapezoid error is small enough to force the result; the integral representation gives no independent constraint.
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