European Physical Journal C: Particles and Fields (Apr 2019)

High-resolution high-speed microwave-multiplexed low temperature microcalorimeters for the HOLMES experiment

  • B. Alpert,
  • D. Becker,
  • D. Bennet,
  • M. Biasotti,
  • M. Borghesi,
  • G. Gallucci,
  • M. De Gerone,
  • M. Faverzani,
  • E. Ferri,
  • J. Fowler,
  • J. Gard,
  • A. Giachero,
  • J. Hays–Wehle,
  • G. Hilton,
  • J. Mates,
  • A. Nucciotti,
  • A. Orlando,
  • G. Pessina,
  • A. Puiu,
  • C. Reintsema,
  • D. Schmidt,
  • D. Swetz,
  • J. Ullom,
  • L. Vale

DOI
https://doi.org/10.1140/epjc/s10052-019-6814-4
Journal volume & issue
Vol. 79, no. 4
pp. 1 – 8

Abstract

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Abstract 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 $$^{163}$$ 163 Ho electron capture spectrum. The detectors required for such an experiment feature a high energy resolution at the Q–value of the transition, around $$\sim $$ ∼ 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 $$^{163}$$ 163 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$$_\alpha $$ α line, at $$\sim $$ ∼ 2.6 keV, obtained with an exponential rise time of 14 $$\upmu $$ μ 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 $$^{163}$$ 163 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.