Direct in-chamber radon-220 (thoron) emanation measurements for rare-event physics experiments

Journal of Instrumentation 21:3 (2026)

Authors:

RR Marcelo Gregorio, F Dastgiri, A Basharina-Freshville, VU Bashu, A Cottle, LJ Bignell, C Ghag, GJ Lane, AG McLean, NJC Spooner

Abstract:

Measuring radon emanation from detector materials is a key method for controlling radon, a significant background in rare-event physics experiments. Methods for measuring radon emanation are well-established but have predominantly focused on the222Rn isotope, the dominant radon isotope for these backgrounds. However, measurements of220Rn (thoron), the second most abundant radon isotope, remain relatively unexplored.220Rn emanation measurements are challenging because the220Rn must be transferred from the emanation chamber to the active detector within its short 55 s half-life. In this study, a direct in-chamber approach for measuring220Rn emanation is presented in which the sample is placed directly within the active detector chamber, thereby minimising losses during transfer. The method was demonstrated with a DURRIDGE RAD8 electrostatic radon detector, which measured220Rn emanation from low-activity thoriated rods with an activity of 76 ± 20 mBq. Compared with a conventional flowthrough220Rn emanation setup, the in-chamber method increased sensitivity by a factor of 3. Using helium as the carrier gas provided a further sensitivity increase, giving an overall sensitivity gain of ∼ 5. These results indicate that in-chamber220Rn emanation measurements provide an effective tool for low-background experiments and have the potential to accelerate radon studies by exploiting the shorter half-life of220Rn.

Production, quality assurance and quality control of the SiPM Tiles for the DarkSide-20k Time Projection Chamber

The European Physical Journal C SpringerOpen 85:11 (2025) 1334

Authors:

F Acerbi, P Adhikari, P Agnes, I Ahmad, S Albergo, IF Albuquerque, T Alexander, AK Alton, P Amaudruz, M Angiolilli, E Aprile, M Atzori Corona, DJ Auty, M Ave, IC Avetisov, O Azzolini, HO Back, Z Balmforth, A Barrado Olmedo, P Barrillon, G Batignani, P Bhowmick, M Bloem, S Blua, V Bocci, W Bonivento, B Bottino, MG Boulay, T Braun, A Buchowicz, S Bussino, J Busto, M Cadeddu, M Cadoni, R Calabrese, V Camillo, A Caminata, N Canci, M Caravati, M Cárdenas-Montes, N Cargioli, M Carlini, A Castellani, P Cavalcante, S Cebrian, S Chashin, A Chepurnov, S Choudhary, L Cifarelli, B Cleveland

Abstract:

Abstract The DarkSide-20k dark matter direct detection experiment will employ a $${21}\,\hbox {m}^{2}$$ 21 m 2 silicon photomultiplier (SiPM) array, instrumenting a dual-phase 50 tonnes liquid argon Time Projection Chamber (TPC). SiPMs are arranged into modular photosensors called Tiles , each integrating 24 SiPMs onto a printed circuit board (PCB) that provides signal amplification, power distribution, and a single-ended output for simplified readout. $$16$$ 16 Tiles are further grouped into Photo-Detector Units (PDUs). This paper details the production of the Tiles and the Quality Assurance and Quality Control (QA-QC) protocol established to ensure their performance and uniformity. The production and QA-QC of the Tiles are carried out at Nuova Officina Assergi (NOA), an ISO-6 clean room facility at LNGS. This process includes wafer-level cryogenic characterisation, precision die attaching, wire bonding, and extensive electrical and optical validation of each Tile. The overall production yield exceeds 83.5%, matching the requirements of the DarkSide-20k production plan. These results validate the robustness of the Tile design and its suitability for operation in a cryogenic environment.

Observation of a low energy nuclear recoil peak in the neutron calibration data of an Al2O3 crystal in CRESST-III

Physical Review D 112:10 (2025) 102008

Authors:

G Angloher, F Casadei, E Cipelli, L Canonica, F Dominsky, D Hauff, A Langenkämper, M Mancuso, B Mauri, C Moore, F Petricca, F Pröbst, K Schäffner, M Stahlberg, L Stodolsky, M Zanirato, A Bento, S Di Lorenzo, D Fuchs, PV Guillaumon, V Zema, J Burkhart, S Fichtinger, VM Ghete, H Kluck, V Mokina, S Banik, L Einfalt, F Reindl, J Schieck, C Schwertner, D Valdenaire, A Bertolini, L Burmeister, E Fascione, P Murali, B von Krosigk, R Breier, M Ješkovský, P Povinec, C Bucci, P Gorla, M Olmi, F Pucci, C Pagliarone, L Pattavina, J Dohm, J Jochum, C Strandhagen, I Usherov, FV Feilitzsch, M Kaznacheeva, T Ortmann, W Potzel, J Rothe, S Schönert, R Strauss, A Erb, H Kraus, M Macko, V Palušovà

Abstract:

The current generation of cryogenic solid state detectors used in direct dark matter and CEνNS searches typically reach energy thresholds of O(10) eV for nuclear recoils. For a reliable calibration in this energy regime a method has been proposed, providing monoenergetic nuclear recoils at low energies ∼100 eV–1 keV. In this work we report on the observation of a peak at (1113.6-6.5+6.5) eV in the data of an Al2O3 crystal in CRESST-III, which was irradiated with neutrons from an AmBe calibration source. We attribute this monoenergetic peak to the radiative capture of thermal neutrons on Al27 and the subsequent deexcitation via single γ emission. We compare the measured results with the outcome of Geant4 simulations and investigate the possibility to make use of this effect for the energy calibration of Al2O3 detectors at low energies. We further investigate the possibility of a shift in the expected energy scale of this effect caused by the creation of defects in the target crystal.

The XLZD Design Book: Towards the Next-Generation Liquid Xenon Observatory for Dark Matter and Neutrino Physics

(2025)

Authors:

XLZD Collaboration, J Aalbers, K Abe, M Adrover, S Ahmed Maouloud, DS Akerib, AK Al Musalhi, F Alder, L Althueser, DWP Amaral, CS Amarasinghe, A Ames, B Andrieu, N Angelides, E Angelino, B Antunovic, E Aprile, HM Araújo, JE Armstrong, M Arthurs, M Babicz, A Baker, M Balzer, J Bang, E Barberio, JW Bargemann, E Barillier, A Basharina-Freshville, L Baudis, D Bauer, M Bazyk, K Beattie, N Beaupere, NF Bell, L Bellagamba, T Benson, A Bhatti, TP Biesiadzinski, R Biondi, Y Biondi, HJ Birch, E Bishop, A Bismark, C Boehm, K Boese, A Bolotnikov, P Brás, R Braun, A Breskin, CAJ Brew, S Brommer, A Brown, G Bruni, R Budnik, S Burdin, C Cai, C Capelli, G Carini, MC Carmona-Benitez, M Carter, A Chauvin, A Chawla, H Chen, JJ Cherwinka, YT Chin, NI Chott, AP Cimental Chavez, K Clark, AP Colijn, DJ Colling, J Conrad, MV Converse, LJ Cooper, R Coronel, D Costanzo, A Cottle, G Cox, JJ Cuenca-García, D Curran, D Cussans, V D'Andrea, LC Daniel Garcia, I Darlington, S Dave, A David, GJ Davies, MP Decowski, A Deisting, J Delgaudio, S Dey, C Di Donato, L Di Felice, P Di Gangi, S Diglio, C Ding, JEY Dobson, M Doerenkamp, G Drexlin, E Druszkiewicz, CL Dunbar, K Eitel, A Elykov, R Engel, SR Eriksen, S Fayer, NM Fearon, AD Ferella, C Ferrari, N Fieldhouse, H Fischer, H Flaecher, T Flehmke, M Flierman, ED Fraser, TMA Fruth, K Fujikawa, W Fulgione, C Fuselli, P Gaemers, R Gaior, RJ Gaitskell, N Gallice, M Galloway, F Gao, N Garroum, A Geffre, J Genovesi, C Ghag, S Ghosh, R Giacomobono, R Gibbons, F Girard, R Glade-Beucke, F Glück, S Gokhale, L Grandi, J Green, J Grigat, MGD van der Grinten, R Größle, H Guan, M Guida, P Gyorgy, JJ Haiston, CR Hall, T Hall, R Hammann, V Hannen, S Hansmann-Menzemer, N Hargittai, E Hartigan-O'Connor, SJ Haselschwardt, M Hernandez, SA Hertel, A Higuera, C Hils, K Hiraoka, L Hoetzsch, M Hoferichter, GJ Homenides, NF Hood, M Horn, DQ Huang, S Hughes, D Hunt, M Iacovacci, Y Itow, E Jacquet, J Jakob, RS James, F Joerg, S Jones, AC Kaboth, F Kahlert, AC Kamaha, Y Kaminaga, M Kara, P Kavrigin, S Kazama, M Keller, P Kemp-Russell, D Khaitan, P Kharbanda, B Kilminster, J Kim, R Kirk, M Kleifges, M Klute, M Kobayashi, D Kodroff, D Koke, A Kopec, EV Korolkova, H Kraus, S Kravitz, L Kreczko, B von Krosigk, VA Kudryavtsev, F Kuger, N Kurita, H Landsman, RF Lang, C Lawes, J Lee, B Lehnert, DS Leonard, KT Lesko, L Levinson, A Li, I Li, S Li, S Liang, Z Liang, J Lin, Y-T Lin, S Lindemann, S Linden, M Lindner, A Lindote, WH Lippincott, K Liu, J Loizeau, F Lombardi, JAM Lopes, MI Lopes, W Lorenzon, M Loutit, C Lu, GM Lucchetti, T Luce, S Luitz, Y Ma, C Macolino, J Mahlstedt, B Maier, PA Majewski, A Manalaysay, A Mancuso, L Manenti, RL Mannino, F Marignetti, T Marley, T Marrodán Undagoitia, K Martens, J Masbou, E Masson, S Mastroianni, C Maupin, V Mazza, C McCabe, ME McCarthy, DN McKinsey, JB McLaughlin, A Melchiorre, J Menéndez, M Messina, EH Miller, B Milosovic, S Milutinovic, K Miuchi, R Miyata, E Mizrachi, A Molinario, CMB Monteiro, ME Monzani, K Morå, S Moriyama, E Morrison, E Morteau, Y Mosbacher, BJ Mount, J Müller, M Murdy, A St J Murphy, M Murra, A Naylor, HN Nelson, F Neves, JL Newstead, A Nguyen, K Ni, J O'Dell, C O'Hare, U Oberlack, M Obradovic, I Olcina, KC Oliver-Mallory, GD Orebi Gann, J Orpwood, S Ouahada, K Oyulmaz, B Paetsch, KJ Palladino, J Palmer, Y Pan, M Pandurovic, NJ Pannifer, S Paramesvaran, SJ Patton, Q Pellegrini, B Penning, G Pereira, R Peres, E Perry, T Pershing, F Piastra, J Pienaar, A Piepke, M Pierre, G Plante, TR Pollmann, F Pompa, L Principe, J Qi, K Qiao, Y Qie, J Qin, S Radeka, V Radeka, M Rajado, D Ramírez García, A Ravindran, A Razeto, J Reichenbacher, CA Rhyne, A Richards, GRC Rischbieter, HS Riyat, R Rosero, A Roy, T Rushton, D Rynders, R Saakyan, L Sanchez, P Sanchez-Lucas, D Santone, JMF dos Santos, G Sartorelli, ABMR Sazzad, A Scaffidi, RW Schnee, J Schreiner, P Schulte, H Schulze Eißing, M Schumann, A Schwenck, A Schwenk, L Scotto Lavina, M Selvi, F Semeria, P Shagin, S Sharma, S Shaw, W Shen, L Sherman, S Shi, SY Shi, T Shimada, T Shutt, JJ Silk, C Silva, H Simgen, G Sinev, R Singh, J Siniscalco, M Solmaz, VN Solovov, Z Song, P Sorensen, J Soria, O Stanley, M Steidl, T Stenhouse, A Stevens, K Stifter, TJ Sumner, A Takeda, P-L Tan, DJ Taylor, WC Taylor, D Thers, T Thümmler, DR Tiedt, F Tönnies, Z Tong, F Toschi, DR Tovey, J Tranter, M Trask, G Trinchero, M Tripathi, DR Tronstad, R Trotta, CD Tunnell, P Urquijo, A Usón, M Utoyama, AC Vaitkus, O Valentino, K Valerius, S Vecchi, V Velan, S Vetter, L de Viveiros, G Volta, D Vorkapic, A Wang, JJ Wang, Y Wang, D Waters, KM Weerman, C Weinheimer, M Weiss, D Wenz, TJ Whitis, K Wild, M Williams, M Wilson, ST Wilson, C Wittweg, J Wolf, FLH Wolfs, S Woodford, D Woodward, M Worcester, CJ Wright, VHS Wu, S Wüstling, M Wurm, Q Xia, Y Xing, D Xu, J Xu, Y Xu, Z Xu, M Yamashita, L Yang, J Ye, M Yeh, B Yu, G Zavattini, W Zha, M Zhong, K Zuber

The XLZD Design Book: towards the next-generation liquid xenon observatory for dark matter and neutrino physics

The European Physical Journal C SpringerOpen 85:10 (2025) 1192

Authors:

J Aalbers, K Abe, M Adrover, S Ahmed Maouloud, DS Akerib, AK Al Musalhi, F Alder, L Althueser, DWP Amaral, CS Amarasinghe, A Ames, B Andrieu, N Angelides, E Angelino, B Antunovic, E Aprile, HM Araújo, JE Armstrong, M Arthurs, M Babicz, A Baker, M Balzer, J Bang, E Barberio

Abstract:

This report describes the experimental strategy and technologies for XLZD, the next-generation xenon observatory sensitive to dark matter and neutrino physics. In the baseline design, the detector will have an active liquid xenon target of 60 tonnes, which could be increased to 80 tonnes if the market conditions for xenon are favorable. It is based on the mature liquid xenon time projection chamber technology used in current-generation experiments, LZ and XENONnT. The report discusses the baseline design and opportunities for further optimization of the individual detector components. The experiment envisaged here has the capability to explore parameter space for Weakly Interacting Massive Particle (WIMP) dark matter down to the neutrino fog, with a 3σ evidence potential for WIMP-nucleon cross sections as low as 3×10-49cm2 (at 40 GeV/c2 WIMP mass). The observatory will also have leading sensitivity to a wide range of alternative dark matter models. It is projected to have a 3σ observation potential of neutrinoless double beta decay of 136Xe at a half-life of up to 5.7×1027 years. Additionally, it is sensitive to astrophysical neutrinos from the sun and galactic supernovae.