The electron capture in $^{163}$Ho experiment – ECHo

Blaum, K.; Chrysalidis, K.; Day Goodacre, T.; Domula, A.; Door, M.; Dorrer, H.; Düllmann, C. E.; Eberhardt, K.; Eliseev, S.; Enss, C.; Faessler, A.; Filianin, P.; Fleischmann, A.; Fonnesu, D.; Gamer, L.; Gastaldo, L.; Haas, R.; Hassel, C.; Hengstler, D.; Jochum, J.; Johnston, K.; Kebschull, U.; Kempf, S.; Kieck, T.; Köster, U.; Lahiri, S.; Maiti, M.; Mantegazzini, F.; Marsh, B.; Neroutsos, P.; Novikov, Y. N.; Ranitzsch, P. C. O.; Rischka, A.; Rothe, S.; Saenz, A.; Sander, O.; Schneider, F.; Scholl, S.; Schweiger, C.; Schüssler, R. X.; Simkovic, F.; Stora, T.; Szücs, Z.; Türler, A.; Veinhard, M.; Weber, M.; Wegner, M.; Wendt, K.; Zuber, K.

The electron capture in $^{163}$ Ho experiment – ECHo

Abstract

Neutrinos, and in particular their tiny but non-vanishing masses, can be considered one of the doors towards physics beyond the Standard Model. Precision measurements of the kinematics of weak interactions, in particular of the

^{3}

H β-decay and the

^{163}

Ho electron capture (EC), represent the only model independent approach to determine the absolute scale of neutrino masses. The electron capture in

^{163}

Ho experiment, ECHo, is designed to reach sub-eV sensitivity on the electron neutrino mass by means of the analysis of the calorimetrically measured electron capture spectrum of the nuclide

^{163}

Ho. The maximum energy available for this decay, about 2.8 keV, constrains the type of detectors that can be used. Arrays of low temperature metallic magnetic calorimeters (MMCs) are being developed to measure the

^{163}

Ho EC spectrum with energy resolution below 3 eV FWHM and with a time resolution below 1 μs. To achieve the sub-eV sensitivity on the electron neutrino mass, together with the detector optimization, the availability of large ultra-pure

^{163}

Ho samples, the identification and suppression of background sources as well as the precise parametrization of the

^{163}

Ho EC spectrum are of utmost importance. The high-energy resolution

^{163}

Ho spectra measured with the first MMC prototypes with ion-implanted

^{163}

Ho set the basis for the ECHo experiment. We describe the conceptual design of ECHo and motivate the strategies we have adopted to carry on the present medium scale experiment, ECHo-1K. In this experiment, the use of 1 kBq

^{163}

Ho will allow to reach a neutrino mass sensitivity below 10 eV/c

^{2}

. We then discuss how the results being achieved in ECHo-1k will guide the design of the next stage of the ECHo experiment, ECHo-1M, where a source of the order of 1 MBq