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 -decay endpoint region with a sensitivity on m_nu of 0.2 hbox {eV}/hbox {c}^2 (90% CL). For this purpose, the upbeta -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 -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 gas mixture at 30 K, as used in the first KATRIN neutrino-mass analyses, as well as a hbox {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}} [1] in the KATRIN neutrino-mass measurement to a subdominant level.

Highlights

  • A background component created from secondary electrons by ion impact on the photocathode adds to the response functions

  • We developed a semi-empirical parametrization for the energyloss function for the scattering of 18.6-keV electrons from hydrogen isotopologs

  • In this paper we report the results of the in-situ measurements of the energy-loss function in the KATRIN experiment

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Summary

Energy-loss function

Multiple processes contribute to the energy loss of electrons traversing molecular tritium gas. Data from detailed measurements is only available for the scattering of 25-keV electrons on molecular hydrogen gas [14,15]; these direct measurements of the energy-loss function were made with energy resolutions down to 40 meV. In these measurements, the contribution of three different groups of lines can be discerned, which are created from the excitations of the (2pσ 1Σu+), (2pπ 1Πu), and (3pπ 1Πu) molecular states around 12.6 eV and 15 eV, respectively. Because of the low energy resolution of several eV, the shape of the energy-loss function was coarsely approximated by a Gaussian to represent electronic excitations and dissociation, and a one-sided Lorentzian to represent the continuum caused by ionization of the molecules [12]

New parametrization
Measurements
Integral measurements
Pile-up correction
Backgrounds
Combined fit of the datasets
Systematic uncertainties
Deuterium results
Findings
Summary and outlook
Full Text
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