- Main
Direct neutrino-mass measurement with sub-electronvolt sensitivity
- Aker, M;
- Beglarian, A;
- Behrens, J;
- Berlev, A;
- Besserer, U;
- Bieringer, B;
- Block, F;
- Bobien, S;
- Böttcher, M;
- Bornschein, B;
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- Brunst, T;
- Caldwell, TS;
- Carney, RMD;
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- Enomoto, S;
- Felden, A;
- Formaggio, JA;
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- Friedel, F;
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- Glück, F;
- Grössle, R;
- Gumbsheimer, R;
- Gupta, V;
- Höhn, T;
- Hannen, V;
- Haußmann, N;
- Helbing, K;
- Hickford, S;
- Hiller, R;
- Hillesheimer, D;
- Hinz, D;
- Houdy, T;
- Huber, A;
- Jansen, A;
- Karl, C;
- Kellerer, F;
- Kellerer, J;
- Kleifges, M;
- Klein, M;
- Köhler, C;
- Köllenberger, L;
- Kopmann, A;
- Korzeczek, M;
- Kovalík, A;
- Krasch, B;
- Krause, H;
- Kunka, N;
- Lasserre, T;
- Le, TL;
- Lebeda, O;
- Lehnert, B;
- Lokhov, A;
- Machatschek, M;
- Malcherek, E;
- Mark, M;
- Marsteller, A;
- Martin, EL;
- Melzer, C;
- Menshikov, A;
- Mertens, S;
- Mostafa, J;
- Müller, K;
- Neumann, H;
- Niemes, S;
- Oelpmann, P;
- Parno, DS;
- Poon, AWP;
- Poyato, JML;
- Priester, F;
- Ramachandran, S;
- Robertson, RGH;
- Rodejohann, W;
- Röllig, M;
- Röttele, C;
- Rodenbeck, C;
- Ryšavý, M;
- Sack, R;
- Saenz, A;
- Schäfer, P;
- Pollithy, A Schaller née;
- Schimpf, L;
- Schlösser, K;
- Schlösser, M;
- Schlüter, L;
- Schneidewind, S;
- Schrank, M;
- Schulz, B;
- Schwemmer, A;
- Šefčík, M;
- Sibille, V;
- Siegmann, D;
- Slezák, M;
- Spanier, F;
- Steidl, M;
- Sturm, M;
- Sun, M;
- Tcherniakhovski, D;
- Telle, HH;
- Thorne, LA;
- Thümmler, T;
- Titov, N;
- Tkachev, I;
- Urban, K;
- Valerius, K;
- Vénos, D;
- Hernández, AP Vizcaya;
- Weinheimer, C;
- Welte, S;
- Wendel, J;
- Wilkerson, JF;
- Wolf, J;
- Wüstling, S;
- Wydra, J;
- Xu, W;
- Yen, Y-R;
- Zadoroghny, S;
- Zeller, G
- et al.
Published Web Location
https://doi.org/10.1038/s41567-021-01463-1Abstract
Since the discovery of neutrino oscillations, we know that neutrinos have non-zero mass. However, the absolute neutrino-mass scale remains unknown. Here we report the upper limits on effective electron anti-neutrino mass, mν, from the second physics run of the Karlsruhe Tritium Neutrino experiment. In this experiment, mν is probed via a high-precision measurement of the tritium β-decay spectrum close to its endpoint. This method is independent of any cosmological model and does not rely on assumptions whether the neutrino is a Dirac or Majorana particle. By increasing the source activity and reducing the background with respect to the first physics campaign, we reached a sensitivity on mν of 0.7 eV c–2 at a 90% confidence level (CL). The best fit to the spectral data yields mν2 = (0.26 ± 0.34) eV2 c–4, resulting in an upper limit of mν < 0.9 eV c–2 at 90% CL. By combining this result with the first neutrino-mass campaign, we find an upper limit of mν < 0.8 eV c–2 at 90% CL.
Main Content
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