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The Triggerless Data Acquisition System of the XENONnT Experiment

Authors :
Aprile, E.
Aalbers, J.
Abe, K.
Agostini, F.
Maouloud, S. Ahmed
Althueser, L.
Andrieu, B.
Angelino, E.
Angevaare, J. R.
Antochi, V. C.
Martin, D. Antón
Arneodo, F.
Baudis, L.
Baxter, A. L.
Bellagamba, L.
Biondi, R.
Bismark, A.
Brookes, E. J.
Brown, A.
Bruenner, S.
Bruno, G.
Budnik, R.
Bui, T. K.
Cai, C.
Cardoso, J. M. R.
Cichon, D.
Chavez, A. P. Cimental
Coderre, D.
Colijn, A. P.
Conrad, J.
Cuenca-García, J. J.
Cussonneau, J. P.
D Andrea, V.
Decowski, M. P.
Di Gangi, P.
Di Pede, S.
Diglio, S.
Eitel, K.
Elykov, A.
Farrell, S.
Ferella, A. D.
Ferrari, C.
Fischer, H.
Flierman, M.
Fulgione, W.
Fuselli, C.
Gaemers, P.
Gaior, R.
Gallo Rosso, A.
Galloway, M.
Gao, F.
Glade-Beucke, R.
Grandi, L.
Grigat, J.
Matteo Guida
Hammann, R.
Higuera, A.
Hils, C.
Hoetzsch, L.
Hood, N. F.
Howlett, J.
Iacovacci, M.
Itow, Y.
Jakob, J.
Joerg, F.
Joy, A.
Kato, N.
Kara, M.
Kavrigin, P.
Kazama, S.
Kobayashi, M.
Koltman, G.
Kopec, A.
Kuger, F.
Landsman, H.
Lang, R. F.
Levinson, L.
Li, I.
Li, S.
Liang, S.
Lindemann, S.
Lindner, M.
Liu, K.
Loizeau, J.
Lombardi, F.
Long, J.
Lopes, J. A. M.
Ma, Y.
Macolino, C.
Mahlstedt, J.
Mancuso, A.
Manenti, L.
Marignetti, F.
Marrodán Undagoitia, T.
Martens, K.
Masbou, J.
Masson, D.
Masson, E.
Mastroianni, S.
Messina, M.
Miuchi, K.
Mizukoshi, K.
Molinario, A.
Moriyama, S.
Morå, K.
Mosbacher, Y.
Murra, M.
Müller, J.
Ni, K.
Oberlack, U.
Paetsch, B.
Palacio, J.
Peres, R.
Peters, C.
Pienaar, J.
Pierre, M.
Pizzella, V.
Plante, G.
Qi, J.
Qin, J.
García, D. Ramírez
Rocchetti, A.
Sanchez, L.
Sanchez-Lucas, P.
Dos Santos, J. M. F.
Sarnoff, I.
Sartorelli, G.
Schreiner, J.
Schulte, D.
Schulte, P.
Eißing, H. Schulze
Schumann, M.
Scotto Lavina, L.
Selvi, M.
Semeria, F.
Shagin, P.
Shi, S.
Shockley, E.
Silva, M.
Simgen, H.
Takeda, A.
Tan, P. -L
Terliuk, A.
Thers, D.
Toschi, F.
Trinchero, G.
Tunnell, C.
Tönnies, F.
Valerius, K.
Volta, G.
Weinheimer, C.
Weiss, M.
Wenz, D.
Wittweg, C.
Wolf, T.
Xu, D.
Xu, Z.
Yamashita, M.
Yang, L.
Ye, J.
Yuan, L.
Zavattini, G.
Zerbo, S.
Zhong, M.
Zhu, T.
HEP, INSPIRE
Source :
INSPIRE-HEP, arXiv

Abstract

The XENONnT detector uses the latest and largest liquid xenon-based timeprojection chamber (TPC) operated by the XENON Collaboration, aimed atdetecting Weakly Interacting Massive Particles and conducting other rare eventsearches. The XENONnT data acquisition (DAQ) system constitutes an upgraded andexpanded version of the XENON1T DAQ system. For its operation, it reliespredominantly on commercially available hardware accompanied by open-source andcustom-developed software. The three constituent subsystems of the XENONnTdetector, the TPC (main detector), muon veto, and the newly introduced neutronveto, are integrated into a single DAQ, and can be operated both independentlyand as a unified system. In total, the DAQ digitizes the signals of 698photomultiplier tubes (PMTs), of which 253 from the top PMT array of the TPCare digitized twice, at $\times10$ and $\times0.5$ gain. The DAQ for the mostpart is a triggerless system, reading out and storing every signal that exceedsthe digitization thresholds. Custom-developed software is used to process theacquired data, making it available within $\mathcal{O}\left(10\text{ s}\right)$for live data quality monitoring and online analyses. The entire system withall the three subsystems was successfully commissioned and has been operatingcontinuously, comfortably withstanding readout rates that exceed $\sim500$ MB/sduring calibration. Livetime during normal operation exceeds $99\%$ and is$\sim90\%$ during most high-rate calibrations. The combined DAQ system hascollected more than 2 PB of both calibration and science data during thecommissioning of XENONnT and the first science run.

Details

Database :
OpenAIRE
Journal :
INSPIRE-HEP, arXiv
Accession number :
edsair.doi.dedup.....df43c3f32c160aa898fcaff6d6621feb