Precision measurement of the electron energy-loss function in tritium and deuterium gas for the KATRIN experiment

  • M. Aker
  • , A. Beglarian
  • , J. Behrens
  • , A. Berlev
  • , U. Besserer
  • , B. Bieringer
  • , F. Block
  • , B. Bornschein
  • , L. Bornschein
  • , M. Böttcher
  • , T. Brunst
  • , T. S. Caldwell
  • , R. M.D. Carney
  • , S. Chilingaryan
  • , W. Choi
  • , K. Debowski
  • , M. Deffert
  • , M. Descher
  • , D. Díaz Barrero
  • , P. J. Doe
  • O. Dragoun, G. Drexlin, F. Edzards, K. Eitel, E. Ellinger, A. El Miniawy, R. Engel, S. Enomoto, A. Felden, J. A. Formaggio, F. M. Fränkle, G. B. Franklin, F. Friedel, A. Fulst, K. Gauda, W. Gil, F. Glück, S. Groh, R. Grössle, R. Gumbsheimer, V. Hannen, N. Haußmann, F. Heizmann, K. Helbing, S. Hickford, R. Hiller, D. Hillesheimer, D. Hinz, T. Höhn, T. Houdy, A. Huber, A. Jansen, C. Karl, J. Kellerer, M. Kleesiek, M. Klein, C. Köhler, L. Köllenberger, A. Kopmann, M. Korzeczek, A. Kovalík, B. Krasch, H. Krause, N. Kunka, T. Lasserre, L. La Cascio, O. Lebeda, B. Lehnert, T. L. Le, A. Lokhov, M. Machatschek, E. Malcherek, M. Mark, A. Marsteller, E. L. Martin, M. Meier, C. Melzer, A. Menshikov, S. Mertens, J. Mostafa, K. Müller, S. Niemes, P. Oelpmann, D. S. Parno, A. W.P. Poon, J. M.L. Poyato, F. Priester, P. C.O. Ranitzsch, R. G.H. Robertson, W. Rodejohann, C. Rodenbeck, M. Röllig, C. Röttele, M. Ryšavý, R. Sack, A. Saenz, P. Schäfer, A. Schaller (née Pollithy), L. Schimpf, K. Schlösser, M. Schlösser, L. Schlüter, S. Schneidewind, M. Schrank, B. Schulz, C. Schwachtgen, M. Šefčík, H. Seitz-Moskaliuk, V. Sibille, D. Siegmann, M. Slezák, M. Steidl, M. Sturm, M. Sun, D. Tcherniakhovski, H. H. Telle, L. A. Thorne, T. Thümmler, N. Titov, I. Tkachev, N. Trost, K. Urban, K. Valerius, D. Vénos, A. P.Vizcaya Hernández, C. Weinheimer, S. Welte, J. Wendel, J. F. Wilkerson, J. Wolf, S. Wüstling, W. Xu, Y. R. Yen, S. Zadoroghny, G. Zeller

Research output: Contribution to journalArticlepeer-review

9 Scopus citations

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 β -decay endpoint region with a sensitivity on mν of 0.2 eV / c 2 (90% CL). For this purpose, the 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 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% T 2 gas mixture at 30 K, as used in the first KATRIN neutrino-mass analyses, as well as a 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 σ(mν2)<10-2eV2 [1] in the KATRIN neutrino-mass measurement to a subdominant level.

Original languageEnglish
Article number579
JournalEuropean Physical Journal C
Volume81
Issue number7
DOIs
StatePublished - Jul 2021

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