First demonstration of a TES based cryogenic Li_2MoO_4detector for neutrinoless double beta decay search

G. Bratrud, C. L. Chang, R. Chen,E. Cudmore,E. Figueroa-Feliciano, Z. Hong,K. T. Kennard, S. Lewis,M. Lisovenko, L. O. Mateo,V. Novati,V. Novosad,E. Oliveri,R. Ren,J. A. Scarpaci, B. Schmidt, G. Wang,L. Winslow,V. G. Yefremenko, J. Zhang,D. Baxter,M. Hollister, C. James, P. Lukens,D. J. Temples

arxiv(2024)

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摘要
Cryogenic calorimetric experiments to search for neutrinoless double-beta decay (0νββ) are highly competitive, scalable and versatile in isotope. The largest planned detector array, CUPID, is comprised of about 1500 individual Li_2^100MoO_4 detector modules with a further scale up envisioned for a follow up experiment (CUPID-1T). In this article, we present a novel detector concept targeting this second stage with a low impedance TES based readout for the Li_2MoO_4 absorber that is easily mass-produced and lends itself to a multiplexed readout. We present the detector design and results from a first prototype detector operated at the NEXUS shallow underground facility at Fermilab. The detector is a 2-cm-side cube with 21g mass that is strongly thermally coupled to its readout chip to allow rise-times of ∼0.5ms. This design is more than one order of magnitude faster than present NTD based detectors and is hence expected to effectively mitigate backgrounds generated through the pile-up of two independent two neutrino decay events coinciding close in time. Together with a baseline resolution of 1.95keV (FWHM) these performance parameters extrapolate to a background index from pile-up as low as 5· 10^-6counts/keV/kg/yr in CUPID size crystals. The detector was calibrated up to the MeV region showing sufficient dynamic range for 0νββ searches. In combination with a SuperCDMS HVeV detector this setup also allowed us to perform a precision measurement of the scintillation time constants of Li_2MoO_4. The crystal showed a significant fast scintillation emission with O(10μs) time-scale, more than an order below the detector response of presently considered light detectors suggesting the possibility of further progress in pile-up rejection through better light detectors in the future.
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