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A quality assurance and performance qualification laboratory was built at McGill University for the Canadian-made small-strip Thin Gap Chamber (sTGC) muon detectors produced for the 2019-2020 ATLAS experiment muon spectrometer upgrade. The…

The EXO-200 experiment searched for neutrinoless double-beta decay of $^{136}$Xe with a single-phase liquid xenon detector. It used an active mass of 110 kg of 80.6%-enriched liquid xenon in an ultra-low background time projection chamber…

Instrumentation and Detectors · Physics 2022-02-23 N. Ackerman , J. Albert , M. Auger , D. J. Auty , I. Badhrees , P. S. Barbeau , L. Bartoszek , E. Baussan , V. Belov , C. Benitez-Medina , T. Bhatta , M. Breidenbach , T. Brunner , G. F. Cao , W. R. Cen , C. Chambers , B. Cleveland , R. Conley , S. Cook , M. Coon , W. Craddock , A. Craycraft , W. Cree , T. Daniels , L. Darroch , S. J. Daugherty , J. Daughhetee , C. G. Davis , J. Davis , S. Delaquis , A. Der Mesrobian-Kabakian , R. deVoe , T. Didberidze , J. Dilling , A. Dobi , A. G. Dolgolenko , M. J. Dolinski , M. Dunford , J. Echevers , L. Espic , W. Fairbank , D. Fairbank , J. Farine , W. Feldmeier , S. Feyzbakhsh , P. Fierlinger , K. Fouts , D. Franco , D. Freytag , D. Fudenberg , P. Gautam , G. Giroux , R. Gornea , K. Graham , G. Gratta , C. Hagemann , C. Hall , K. Hall , G. Haller , E. V. Hansen , C. Hargrove , R. Herbst , S. Herrin , J. Hodgson , M. Hughes , A. Iverson , A. Jamil , C. Jessiman , M. J. Jewell , A. Johnson , T. N. Johnson , S. Johnston , A. Karelin , L. J. Kaufman , R. Killick , T. Koffas , S. Kravitz , R. Krücken , A. Kuchenkov , K. S. Kumar , Y. Lan , A. Larson , D. S. Leonard , F. Leonard , F. LePort , G. S. Li , S. Li , Z. Li , C. Licciardi , Y. H. Lin , D. Mackay , R. MacLellan , M. Marino , J. -M. Martin , Y. Martin , T. McElroy , K. McFarlane , T. Michel , B. Mong , D. C. Moore , K. Murray , R. Neilson , O. Njoya , O. Nusair , K. O'Sullivan , A. Odian , I. Ostrovskiy , C. Ouellet , A. Piepke , A. Pocar , C. Y. Prescott , K. Pushkin , F. Retiere , A. Rivas , A. L. Robinson , E. Rollin , P. C. Rowson , M. P. Rozo , J. Runge , J. J. Russell , S. Schmidt , A. Schubert , D. Sinclair , K. Skarpaas , S. Slutsky , E. Smith , A. K. Soma , V. Stekhanov , V. Strickland , M. Swift , M. Tarka , J. Todd , T. Tolba , D. Tosi , T. I. Totev , R. Tsang , K. Twelker , B. Veenstra , V. Veeraraghavan , J. -L. Vuilleumier , J. -M. Vuilleumier , M. Wagenpfeil , A. Waite , J. Walton , T. Walton , K. Wamba , J. Watkins , M. Weber , L. J. Wen , U. Wichoski , M. Wittgen , J. Wodin , J. Wood , G. Wrede , S. X. Wu , Q. Xia , L. Yang , Y. -R. Yen , O. Ya Zeldovich , T. Ziegler

For the sake of saving time and costs the feedback control based on discrete-time observations is used to stabilize the switching diffusion systems. Response lags are required by most of physical systems and play a key role in the feedback…

Optimization and Control · Mathematics 2020-08-20 Xiaoyue Li , Xuerong Mao , Denis S. Mukama , Chenggui Yuan

The design of the project named CYGNO is presented. CYGNO is a new proposal supported by INFN, the Italian National Institute for Nuclear Physics, within CYGNUs proto-collaboration (CYGNUS-TPC) that aims to realize a distributed observatory…

Detector control systems (DCS) include the read out, control and supervision of hardware devices as well as the monitoring of external systems like cooling system and the processing of control data. The implementation of such a system in…

Instrumentation and Detectors · Physics 2009-11-11 Martin Imhaeuser , Karl-Heinz Becks , Tobias Henss , Susanne Kersten , Peter Maettig , Joachim Schultes

Dual-phase liquid xenon time projection chambers are the core detector elements of many experiments that conduct searches for Dark Matter and rare events, as well as in neutrino and high-energy physics. As part of this detector technology,…

The NEXT collaboration is dedicated to the study of double beta decays of $^{136}$Xe using a high-pressure gas electroluminescent time projection chamber. This advanced technology combines exceptional energy resolution ($\leq 1\%$ FWHM at…

Instrumentation and Detectors · Physics 2026-02-12 NEXT Collaboration , C. Adams , H. Almazán , V. Álvarez , A. I. Aranburu , L. Arazi , I. J. Arnquist , F. Auria-Luna , S. Ayet , Y. Ayyad , C. D. R. Azevedo , K. Bailey , F. Ballester , J. E. Barcelon , M. del Barrio-Torregrosa , A. Bayo , J. M. Benlloch-Rodríguez , F. I. G. M. Borges , A. Brodoline , N. Byrnes , A. Castillo , E. Church , L. Cid , M. Cid , X. Cid , C. A. N. Conde , C. Cortes-Parra , F. P. Cossío , R. Coupe , E. Dey , P. Dietz , C. Echeverria , M. Elorza , R. Esteve , R. Felkai , L. M. P. Fernandes , P. Ferrario , F. W. Foss , Z. Freixa , J. García-Barrena , J. J. Gómez-Cadenas , J. W. R. Grocott , R. Guenette , J. Hauptman , C. A. O. Henriques , J. A. Hernando Morata , P. Herrero-Gómez , V. Herrero , C. Hervés Carrete , Y. Ifergan , A. F. B. Isabel , B. J. P. Jones , F. Kellerer , L. Larizgoitia , A. Larumbe , P. Lebrun , F. Lopez , N. López-March , R. Madigan , R. D. P. Mano , A. Marauri , A. P. Marques , J. Martín-Albo , A. Martínez , G. Martínez-Lema , M. Martínez-Vara , R. L. Miller , K. Mistry , J. Molina-Canteras , F. Monrabal , C. M. B. Monteiro , F. J. Mora , K. E. Navarro , P. Novella , D. R. Nygren , E. Oblak , I. Osborne , J. Palacio , B. Palmeiro , A. Para , I. Parmaksiz , A. Pazos , J. Pelegrin , M. Pérez Maneiro , M. Querol , J. Renner , I. Rivilla , C. Rogero , L. Rogers , B. Romeo , C. Romo-Luque , E. Ruiz-Chóliz , P. Saharia , F. P. Santos , J. M. F. dos Santos , M. Seemann , I. Shomroni , A. L. M. Silva , P. A. O. C. Silva , A. Simón , S. R. Soleti , M. Sorel , J. Soto-Oton , J. M. R. Teixeira , S. Teruel-Pardo , J. F. Toledo , C. Tonnelé , S. Torelli , J. Torrent , A. Trettin , P. R. G. Valle , M. Vanga , P. Vázquez Cabaleiro , J. F. C. A. Veloso , J. D. Villamil , J. Waiton , A. Yubero-Navarro

Liquid xenon time-projection chambers are the world's most sensitive detectors for a wide range of dark matter candidates. We show that the statistical analysis of their data can be improved by replacing detector response Monte Carlo…

Instrumentation and Detectors · Physics 2020-11-04 J. Aalbers , B. Pelssers , V. C. Antochi , P. L. Tan , J. Conrad

Making material experiments more efficient is a high priority for materials scientists who seek to discover new materials with desirable properties. In this paper, we investigate how to optimize the laborious sequential measurements of…

Materials Science · Physics 2019-10-24 Takuya Kanazawa , Akinori Asahara , Hidekazu Morita

SPES (Study for the Production of Exotic Species) is a LNL project that will produce by the end of this year the conceptual design of a specialized facility for Radioactive Ion Beam (RIB) originated by fission fragments produced by…

Accelerator Physics · Physics 2007-05-23 Stefania Canella , Giorgio Bassato

The Sodium iodide Active Background Rejection Experiment-South (SABRE-South) is a direct dark matter detector soon to be deployed in the Stawell gold mine, in Victoria, Australia. Monitoring of external environmental and experimental…

Instrumentation and Detectors · Physics 2021-10-04 S. Krishnan , S. Collins , D. Smoors , C. Webster , T. Baroncelli , G. Brooks , J. Mould , W. J. Dix , P. McNamara , F. Scutti , G. Lane , P. Urquijo , A. R. Duffy

Results from the nuclear recoil calibration of the XENON100 dark matter detector installed underground at the Laboratori Nazionali del Gran Sasso (LNGS), Italy are presented. Data from measurements with an external 241AmBe neutron source…

We study in detail sub-GeV dark matter scattering off electrons in xenon, including the expected electron recoil spectra and annual modulation spectra. We derive improved constraints using low-energy XENON10 and XENON100 ionization-only…

High Energy Physics - Phenomenology · Physics 2017-09-06 Rouven Essig , Tomer Volansky , Tien-Tien Yu

The COSINE-100 experiment is designed to test the DAMA experiment which claimed an observation of a dark matter signal from an annual modulation in their residual event rate. To measure the 1 %-level signal amplitude, it is crucial to…

The Run Control and Monitor System (RCMS) of the CMS experiment is the set of hardware and software components responsible for controlling and monitoring the experiment during data-taking. It provides users with a "virtual counting room",…

A low-background germanium spectrometer has been installed and is being operated in an ultra-low background shield (the Gator facility) at the Gran Sasso underground laboratory in Italy (LNGS). With an integrated rate of ~0.16 events/min in…

Instrumentation and Methods for Astrophysics · Physics 2015-05-27 L. Baudis , A. D. Ferella , A. Askin , J. Angle , E. Aprile , T. Bruch , A. Kish , M. Laubenstein , A. Manalaysay , T. Marrodan Undagoitia , M. Schumann

XENON is a dark matter direct detection project, consisting of a time projection chamber (TPC) filled with liquid xenon as detection medium. The construction of the next generation detector, XENON1T, is presently taking place at the…

We investigate a control technique for spatially extended systems combining spatial filtering with a previously studied form of time-delay feedback. The scheme is naturally suited to real-time control of optical systems. We apply the…

The search for dark matter is one of today's most exciting fields. As bigger detectors are being built to increase their sensitivity, background reduction is an ever more challenging issue. To this end, a new type of dark matter detector is…

Instrumentation and Methods for Astrophysics · Physics 2016-03-11 C. Levy , S. Fallon , J. Genovesi , D. Khaitan , K. Klimov , J. Mock , M. Szydagis

The COSINUS (Cryogenic Observatory for SIgnatures seen in Next-generation Underground Searches) experiment aims at the detection of dark matter-induced recoils in sodium iodide (NaI) crystals operated as scintillating cryogenic…