Determining the neutrino mass with Cyclotron Radiation Emission Spectroscopy - Project 8
JPhysG 44 (2017) 5 The most sensitive direct method to establish the absolute neutrino mass is observation of the endpoint of the tritium beta-decay spectrum. Cyclotron Radiation Emission Spectroscopy (CRES) is a precision spectrographic technique that can probe much of the unexplored neutrino mass...
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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Format: | Journal Article |
Language: | English |
Published: |
06-03-2017
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Subjects: | |
Online Access: | Get full text |
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Summary: | JPhysG 44 (2017) 5 The most sensitive direct method to establish the absolute neutrino mass is
observation of the endpoint of the tritium beta-decay spectrum. Cyclotron
Radiation Emission Spectroscopy (CRES) is a precision spectrographic technique
that can probe much of the unexplored neutrino mass range with
$\mathcal{O}({\rm eV})$ resolution. A lower bound of $m(\nu_e) \gtrsim 9(0.1)\,
{\rm meV}$ is set by observations of neutrino oscillations, while the KATRIN
Experiment - the current-generation tritium beta-decay experiment that is based
on Magnetic Adiabatic Collimation with an Electrostatic (MAC-E) filter - will
achieve a sensitivity of $m(\nu_e) \lesssim 0.2\,{\rm eV}$. The CRES technique
aims to avoid the difficulties in scaling up a MAC-E filter-based experiment to
achieve a lower mass sensitivity. In this paper we review the current status of
the CRES technique and describe Project 8, a phased absolute neutrino mass
experiment that has the potential to reach sensitivities down to $m(\nu_e)
\lesssim 40\,{\rm meV}$ using an atomic tritium source. |
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DOI: | 10.48550/arxiv.1703.02037 |