Precision measurement of the electron energy-loss function in tritium and deuterium gas for the KATRIN experiment
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Author(s) • • • • • • • • •
Aker, M.
Beglarian, A.
Behrens, J.
Berlev, A.
Besserer, U.
Bieringer, B.
Block, F.
Bornschein, B.
Bornschein, L.
Böttcher, M.
Date Issued
July 5, 2021
Publisher
Springer Berlin Heidelberg
Citation
The European Physical Journal C. 2021 Jul 05;81(7):579
Version
Final published version
Abstract
Abstract
The KATRIN experiment is designed for a direct and model-independent determination of the effective electron anti-neutrino mass via a high-precision measurement of the tritium
$$\upbeta $$
β
-decay endpoint region with a sensitivity on
$$m_\nu $$
m
ν
of 0.2
$$\hbox {eV}/\hbox {c}^2$$
eV
/
c
2
(90% CL). For this purpose, the
$$\upbeta $$
β
-electrons from a high-luminosity windowless gaseous tritium source traversing an electrostatic retarding spectrometer are counted to obtain an integral spectrum around the endpoint energy of 18.6 keV. A dominant systematic effect of the response of the experimental setup is the energy loss of
$$\upbeta $$
β
-electrons from elastic and inelastic scattering off tritium molecules within the source. We determined the energy-loss function in-situ with a pulsed angular-selective and monoenergetic photoelectron source at various tritium-source densities. The data was recorded in integral and differential modes; the latter was achieved by using a novel time-of-flight technique. We developed a semi-empirical parametrization for the energy-loss function for the scattering of 18.6-keV electrons from hydrogen isotopologs. This model was fit to measurement data with a 95%
$$\hbox {T}_2$$
T
2
gas mixture at 30 K, as used in the first KATRIN neutrino-mass analyses, as well as a
$$\hbox {D}_2$$
D
2
gas mixture of 96% purity used in KATRIN commissioning runs. The achieved precision on the energy-loss function has abated the corresponding uncertainty of
$$\sigma (m_\nu ^2)< {{10}^{-2}}{\hbox {eV}^{2}}$$
σ
(
m
ν
2
)
<
10
-
2
eV
2
[1] in the KATRIN neutrino-mass measurement to a subdominant level.
MIT Department
Massachusetts Institute of Technology. Laboratory for Nuclear Science
Massachusetts Institute of Technology. Department of Physics
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DOI of Published Version
https://doi.org/10.1140/epjc/s10052-021-09325-z