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The reconstruction of the positron trajectory in the MEG-II experiment searching for the $\mu^+ \to e^+ \gamma$ decay uses a cylindrical drift chamber operated with a helium-isobutane gas mixture. A stable performance of the detector in…

High-energy neutrino flares are interesting prospective counterparts to photon flares, as their detection would guarantee the presence of accelerated hadrons within a source, provide precious information about cosmic-ray acceleration and…

High Energy Astrophysical Phenomena · Physics 2020-09-02 Claire Guépin

The CALICE Semi-Digital Hadron Calorimeter technological prototype completed in 2011 is a sampling calorimeter using Glass Resistive Plate Chamber (GRPC) detectors as the active medium. This technology is one of the two options proposed for…

A new type of gaseous micropattern particle detector based on a closed-cell microcavity plasma panel sensor is reported. The first device was fabricated with 1 x 1 x 2 mm cells. It has shown very clean signals of 0.6 to 2.5 volt amplitude,…

Various phase shifters and absorbers can be put into the arms of a double loop neutron interferometer. The mean intensity levels of the forward and diffracted beams behind an empty four plate interferometer of this type have been…

Quantum Physics · Physics 2009-11-10 M. Suda , H. Rauch , M. Peev

A Computationally Assisted Spectroscopic Technique to measure secondary electron emission coefficients ($\gamma$-CAST) in capacitively-coupled radio-frequency plasmas is proposed. This non-intrusive, sensitive diagnostic is based on a…

Plasma Physics · Physics 2016-06-22 M. Daksha , B. Berger , E. Schuengel , I. Korolov , A. Derzsi , M. Koepke , Z. Donko , J. Schulze

Modern approaches to the detection and imaging of rare particle interactions through gaseous and dual-phase time projection chambers are discussed. We introduce and examine their basic working principles and enabling technological assets.

Instrumentation and Detectors · Physics 2018-03-14 D. Gonzalez-Diaz , F. Monrabal , S. Murphy

This communication describes test beam results, focusing on detection efficiency and timing precision, of common float glass timing Resistive Plate Chambers (tRPCs) exposed to a $2.7$~GeV proton beam and operated at above ambient…

Instrumentation and Detectors · Physics 2022-11-23 A. Blanco , P. Fonte , L. Lopes , J. Saraiva

The CALICE collaboration is currently developing an engineering prototype of an analog hadron calorimeter for a future linear collider detector. It is based on scintillating tiles that are individually read out by silicon photomultipliers.…

Instrumentation and Detectors · Physics 2019-08-14 Mark Terwort

The SDHCAL technological prototype is a $1 \times 1 \times 1.3$~m$^3$ high-granularity Semi-Digital Hadronic CALorimeter using Glass Resistive Plate Chambers as sensitive medium. It is one of the two HCAL options considered by the ILD…

Instrumentation and Detectors · Physics 2016-08-03 Gérald Grenier

The Phase II upgrade of the ATLAS Muon Spectrometer will involve the installation of approximately 1000 next-generation Resistive Plate Chamber (RPC) singlets. This upgrade aims to enhance detector coverage, increase hit efficiency, and…

Instrumentation and Detectors · Physics 2025-06-23 Aashaq Shah

Primary cosmic rays when interact with our atmosphere, produce a cascade of lighter secondary particles namely pion, kaon, neutrons, muons, electrons, positrons and neutrinos. Muons are one of the most abundant and easily detectable…

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

The Liquid Argon Time Projection Chamber offers an innovative technology for a new class of massive detectors for rare-event detection. It is a precise tracking device that allows three-dimensional spatial reconstruction with mm-scale…

Instrumentation and Detectors · Physics 2015-06-15 A. Rubbia

We extend our recent analysis of the dilepton and photon emission rates to the case of finite temperature and baryon density, within the context of a density expansion. To leading order, the effects of the baryon density are assessed using…

High Energy Physics - Phenomenology · Physics 2014-11-17 James V. Steele , Hidenaga Yamagishi , Ismail Zahed

The semi-digital Hadronic calorimeter using GRPC as sensitive medium is one of the two options the ILD collaboration is considering for the ILD detector final design. A prototype of 1m3 has been conceived within the CALICE collaboration in…

Instrumentation and Detectors · Physics 2019-08-13 N. Lumb

The Compact Muon Solenoid Collaboration is designing a new high-granularity endcap calorimeter, HGCAL, to be installed later this decade. As part of this development work, a prototype system was built, with an electromagnetic section…

Instrumentation and Detectors · Physics 2022-05-25 B. Acar , G. Adamov , C. Adloff , S. Afanasiev , N. Akchurin , B. Akgün , F. Alam Khan , M. Alhusseini , J. Alison , A. Alpana , G. Altopp , M. Alyari , S. An , S. Anagul , I. Andreev , P. Aspell , I. O. Atakisi , O. Bach , A. Baden , G. Bakas , A. Bakshi , S. Bannerjee , P. Bargassa , D. Barney , F. Beaudette , F. Beaujean , E. Becheva , A. Becker , P. Behera , A. Belloni , T. Bergauer , M. Besancon , S. Bhattacharya , D. Bhowmik , B. Bilki , P. Bloch , A. Bodek , M. Bonanomi , A. Bonnemaison , S. Bonomally , J. Borg , F. Bouyjou , N. Bower , D. Braga , J. Brashear , E. Brondolin , P. Bryant , A. Buchot Perraguin , J. Bueghly , B. Burkle , A. Butler-Nalin , O. Bychkova , S. Callier , D. Calvet , X. Cao , A. Cappati , B. Caraway , S. Caregari , A. Cauchois , L. Ceard , Y. C. Cekmecelioglu , S. Cerci , G. Cerminara , M. Chadeeva , N. Charitonidis , R. Chatterjee , Y. M. Chen , Z. Chen , H. J. Cheng , K. y. Cheng , S. Chernichenko , H. Cheung , C. H. Chien , S. Choudhury , D. Čoko , G. Collura , F. Couderc , M. Danilov , D. Dannheim , W. Daoud , P. Dauncey , A. David , G. Davies , O. Davignon , E. Day , P. DeBarbaro , F. De Guio , C. de La Taille , M. De Silva , P. Debbins , M. M. Defranchis , E. Delagnes , J. M. Deltoro Berrio , G. Derylo , P. G. Dias de Almeida , D. Diaz , P. Dinaucourt , J. Dittmann , M. Dragicevic , S. Dugad , F. Dulucq , I. Dumanoglu , V. Dutta , S. Dutta , M. Dünser , J. Eckdahl , T. K. Edberg , M. El Berni , F. Elias , S. C. Eno , Yu. Ershov , P. Everaerts , S. Extier , F. Fahim , C. Fallon , G. Fedi , B. A. Fontana Santos Alves , E. Frahm , G. Franzoni , J. Freeman , T. French , P. Gandhi , S. Ganjour , X. Gao , A. Garcia-Bellido , F. Gastaldi , Z. Gecse , Y. Geerebaert , H. Gerwig , O. Gevin , S. Ghosh , A. Gilbert , W. Gilbert , K. Gill , C. Gingu , S. Gninenko , A. Golunov , I. Golutvin , T. Gonzalez , N. Gorbounov , L. Gouskos , A. B. Gray , Y. Gu , F. Guilloux , Y. Guler , E. Gülmez , J. Guo , E. Gurpinar Guler , M. Hammer , H. M. Hassanshahi , K. Hatakeyama , A. Heering , V. Hegde , U. Heintz , N. Hinton , J. Hirschauer , J. Hoff , W. -S. Hou , X. Hou , H. Hua , J. Incandela , A. Irshad , C. Isik , S. Jain , H. R. Jheng , U. Joshi , V. Kachanov , A. Kalinin , L. Kalipoliti , A. Kaminskiy , A. Kapoor , O. Kara , A. Karneyeu , M. Kaya , O. Kaya , A. Kayis Topaksu , A. Khukhunaishvili , J. Kiesler , M. Kilpatrick , S. Kim , K. Koetz , T. Kolberg , O. K. Köseyan , A. Kristić , M. Krohn , K. Krüger , N. Kulagin , S. Kulis , S. Kunori , C. M. Kuo , V. Kuryatkov , S. Kyre , Y. Lai , K. Lamichhane , G. Landsberg , C. Lange , J. Langford , M. Y. Lee , A. Levin , A. Li , B. Li , J. H. Li , Y. y. Li , H. Liao , D. Lincoln , L. Linssen , R. Lipton , Y. Liu , A. Lobanov , R. -S. Lu , M. Lupi , I. Lysova , A. -M. Magnan , F. Magniette , A. Mahjoub , A. A. Maier , A. Malakhov , S. Mallios , I. Mandjavize , M. Mannelli , J. Mans , A. Marchioro , A. Martelli , G. Martinez , P. Masterson , B. Meng , T. Mengke , A. Mestvirishvili , I. Mirza , S. Moccia , G. B. Mohanty , F. Monti , I. Morrissey , S. Murthy , J. Musić , Y. Musienko , S. Nabili , A. Nagar , M. Nguyen , A. Nikitenko , D. Noonan , M. Noy , K. Nurdan , C. Ochando , B. Odegard , N. Odell , H. Okawa , Y. Onel , W. Ortez , J. Ozegović , S. Ozkorucuklu , E. Paganis , D. Pagenkopf , V. Palladino , S. Pandey , F. Pantaleo , C. Papageorgakis , I. Papakrivopoulos , J. Parshook , N. Pastika , M. Paulini , P. Paulitsch , T. Peltola , R. Pereira Gomes , H. Perkins , P. Petiot , T. Pierre-Emile , F. Pitters , E. Popova , H. Prosper , M. Prvan , I. Puljak , H. Qu , T. Quast , R. Quinn , M. Quinnan , M. T. Ramos Garcia , K. K. Rao , K. Rapacz , L. Raux , G. Reichenbach , M. Reinecke , M. Revering , A. Roberts , T. Romanteau , A. Rose , M. Rovere , A. Roy , P. Rubinov , R. Rusack , V. Rusinov , V. Ryjov , O. M. Sahin , R. Salerno , A. M. Sanchez Rodriguez , R. Saradhy , T. Sarkar , M. A. Sarkisla , J. B. Sauvan , I. Schmidt , M. Schmitt , E. Scott , C. Seez , F. Sefkow , S. Sharma , I. Shein , A. Shenai , R. Shukla , E. Sicking , P. Sieberer , P. Silva , A. E. Simsek , Y. Sirois , V. Smirnov , U. Sozbilir , E. Spencer , A. Steen , J. Strait , N. Strobbe , J. W. Su , E. Sukhov , L. Sun , D. Sunar Cerci , C. Syal , B. Tali , C. L. Tan , J. Tao , I. Tastan , T. Tatli , R. Thaus , S. Tekten , D. Thienpont , E. Tiras , M. Titov , D. Tlisov , U. G. Tok , J. Troska , L. -S. Tsai , Z. Tsamalaidze , G. Tsipolitis , A. Tsirou , N. Tyurin , S. Undleeb , D. Urbanski , V. Ustinov , A. Uzunian , M. Van de Klundert , J. Varela , M. Velasco , O. Viazlo , M. Vicente Barreto Pinto , P. Vichoudis T. Virdee , R. Vizinho de Oliveira , J. Voelker , E. Voirin , M. Vojinovic , A. Wade , C. Wang , F. Wang , X. Wang , Z. Wang , Z. Wang , M. Wayne , S. N. Webb , A. Whitbeck , D. White , R. Wickwire , J. S. Wilson , D. Winter , H. y. Wu , L. Wu , M. Wulansatiti Nursanto , C. H Yeh , R. Yohay , D. Yu , G. B. Yu , S. S. Yu , C. Yuan , F. Yumiceva , I. Yusuff , A. Zacharopoulou , N. Zamiatin , A. Zarubin , S. Zenz , A. Zghiche , H. Zhang , J. Zhang , Y. Zhang , Z. Zhang

The paper describes the SPHINX facility which includes a wide-aperture magnetic spectrometer with scintillation counters and hodoscopes, proportional chambers and drift tubes, multichannel electromagnetic and hadron calorimeters, a guard…

We discuss the design and performance of a threshold Cerenkov counter for identification of charged hadrons. The radiator is pressurized gas, which is contained in thin-walled cylindrical modules. A mirror system of novel design transports…

High Energy Physics - Experiment · Physics 2008-11-26 Michael Sivertz , Bruce Berger , Richard Ehrlich , John Bartlet , Steven Csorna , Vivek Jain , Szabolcs Marka , Kay Kinoshita , Paula Pomianowski

This paper reports on detailed measurements of the performance of Resistive Plate Chambers in a proton beam with variable intensity. Short term effects, such as dead time, are studied using consecutive events. On larger time scales, for…

Instrumentation and Detectors · Physics 2009-06-25 B. Bilki , J. Butler , E. May , G. Mavromanolakis , E. Norbeck , J. Repond , D. Underwood , L. Xia , Q. Zhang