https://doi.org/10.1140/epjc/s10052-019-6814-4
Regular Article - Experimental Physics
High-resolution high-speed microwave-multiplexed low temperature microcalorimeters for the HOLMES experiment
1
National Institute of Standards and Technology (NIST), Boulder, CO, 80305, USA
2
Istituto Nazionale di Fisica Nucleare (INFN), Sezione di Genova, Genoa, 16146, Italy
3
Dipartimento di Fisica “G. Occhialini”, Università di Milano - Bicocca, Milan, 20126, Italy
4
Istituto Nazionale di Fisica Nucleare (INFN), Sezione di Milano-Bicocca, Milan, 20126, Italy
5
Present address: NASA Goddard Space Flight Center, Greenbelt, MD, 20771, USA
6
Present address: Cardiff University, Cardiff, CF24 3AA, UK
* e-mail: marco.faverzani@mib.infn.it
Received:
23
November
2018
Accepted:
28
March
2019
Published online:
4
April
2019
We present the first performance results obtained with microwave multiplexed Transition Edge Sensors prototypes specifically designed for the HOLMES experiment, a project aimed at directly measuring the electron neutrino mass through the calorimetric measurement of the Ho electron capture spectrum. The detectors required for such an experiment feature a high energy resolution at the Q–value of the transition, around 2.8 keV, and a fast response time combined with the compatibility to be multiplexed in large arrays in order to collect a large statistics while keeping the pile-up contribution as small as possible. In addition, the design has to be suitable for future ion-implantation of Ho. The results obtained in these tests allowed us to identify the optimal detector design among several prototypes. The chosen detector achieved an energy resolution of (4.5 ± 0.3) eV on the chlorine K line, at 2.6 keV, obtained with an exponential rise time of 14 s. The achievements described in this paper pose a milestone for the HOLMES detectors, setting a baseline for the subsequent developments, aiming to the actual ion-implantation of the Ho nuclei. In the first section the HOLMES experiment is outlined along with its physics goal, while in the second section the HOLMES detectors are described; the experimental set-up and the calibration source used for the measurements described in this paper are reported in Sects. 3 and 4, respectively; finally, the details of the data analysis and the results obtained are reported in Sect. 6.
© The Author(s), 2019