Eco-friendly resistive plate chamber detectors for HEP applications

Resistive Plate Chamber detectors are largely employed in current High Energy Physics experiments, thanks to their relatively low cost and good spatial/time resolution. They are typically operated in avalanche mode with large fractions of Tetrafluoroethane (C 2 H 2 F 4 ), a gas recently banned by the European Union due to its high Global Warming Potential (GWP). An intense R&D activity is ongoing to improve RPC technology in view of present and future High Energy Particle Physics (HEP) applications. Since a few years, a joint effort among the ALICE, ATLAS, CMS, LHCb/SHiP and CERN Detector Technology (EP-DT) Communities is in place to search for potential eco-friendly gas mixtures and assess the performance of RPCs under different irradiation conditions. Tests are in progress at the CERN Gamma Irradiation Facility (GIF++). In this paper, a review on the promising results of these studies and future plans will be given.

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Publication Details

Journal
International Journal of Modern Physics A
Published
2024-12-20
DOI
https://doi.org/10.1142/s0217751x25410027
Citations
1
Primary Topic
Gas Sensing Nanomaterials and Sensors
Type
article
Field-Weighted Citation Impact
0.21
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article

Eco-friendly resistive plate chamber detectors for HEP applications

M. Romano, B. Joly, R. Cardarelli, D. Piccolo et al.
1 citations
International Journal of Modern Physics A
Gas Sensing Nanomaterials and Sensors
0.21
article

Eco-friendly resistive plate chamber detectors for HEP applications

M. Romano, B. Joly, R. Cardarelli, D. Piccolo, G. Rigoletti, J. Eysermans, P. Dupieux, A. Rocchi, S.P. Manen, A. Polini, D. Boscherini, N. Zaganidis, P. Camarri, E. Pastori, B. Liberti, L. Benussi, A. Di Ciaccio, R. Santonico, G. Saviano, G. Proto, L. Massa, G. Aielli, S. Bianco, Marta F. Barroso, S. Simone, M. Gagliardi, M. Verzeroli, G. Galati, L. Di Stante, R. Aly, Livia Terlizzi, E. Vercellin, B. Mandelli, A. Samalan, M.C. Arena, R. Guida, D. Ramos, A. Bruni, L. Congedo, P. Salvini, G. Pugliese, M. De Serio, M. Tytgat, A. Ferretti, L. Pizzimento, A. Pastore, L. Quaglia, S. Buontempo, M. Abbrescia
article en
1 citations

Abstract

Resistive Plate Chamber detectors are largely employed in current High Energy Physics experiments, thanks to their relatively low cost and good spatial/time resolution. They are typically operated in avalanche mode with large fractions of Tetrafluoroethane (C 2 H 2 F 4 ), a gas recently banned by the European Union due to its high Global Warming Potential (GWP). An intense R&D activity is ongoing to improve RPC technology in view of present and future High Energy Particle Physics (HEP) applications. Since a few years, a joint effort among the ALICE, ATLAS, CMS, LHCb/SHiP and CERN Detector Technology (EP-DT) Communities is in place to search for potential eco-friendly gas mixtures and assess the performance of RPCs under different irradiation conditions. Tests are in progress at the CERN Gamma Irradiation Facility (GIF++). In this paper, a review on the promising results of these studies and future plans will be given.

International Journal of Modern Physics AVol. 40(08)
Université Claude Bernard Lyon 1 (FR), Centre National de la Recherche Scientifique (FR), Université Clermont Auvergne (FR), Ghent University (BE), Universidade do Estado do Rio de Janeiro (BR), Istituto Nazionale di Fisica Nucleare, Sezione di Torino (IT), Laboratoire de Physique de Clermont Auvergne (FR), Istituto Nazionale di Fisica Nucleare, Sezione di Napoli (IT), Istituto Nazionale di Fisica Nucleare, Sezione di Pavia (IT), IIT@MIT (US), Istituto Nazionale di Fisica Nucleare, Sezione di Bari (IT), Istituto Nazionale di Fisica Nucleare, Roma Tor Vergata (IT), Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali di Frascati (IT), Clermont Université (FR), Istituto Nazionale di Fisica Nucleare, Sezione di Bologna (IT), European Organization for Nuclear Research (CH), Universidade Federal do Estado do Rio de Janeiro (BR)
Openalex Percentile: Top 45%
Gas Sensing Nanomaterials and Sensors
0.21
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