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The Tile Calorimeter (TileCal) is the hadronic calorimeter covering the most central region of the ATLAS experiment at LHC. The TileCal readout consists of about 10000 channels. The ATLAS upgrade program is divided in three phases: The…

Instrumentation and Detectors · Physics 2013-05-07 A. S. Cerqueira

A small prototype of a finely granulated digital hadron calorimeter with Resistive Plate Chambers as active elements was exposed to positrons of 1 . 16 GeV energy from the Fermilab test beam. The response function, energy resolution, as…

Instrumentation and Detectors · Physics 2010-06-29 Burak Bilki , John Butler , Ed May , Georgios Mavromanolakis , Edwin Norbeck , Jose Repond , David Underwood , Lei Xia , Qingmin Zhang

A novel technique for longitudinal segmentation of shashlik calorimeters has been tested in the CERN West Area beam facility. A 25 tower very fine samplings e.m. calorimeter has been built with vacuum photodiodes inserted in the first 8…

A highly granular silicon-tungsten electromagnetic calorimeter (SiW-ECAL) is the reference design of the ECAL for International Large Detector concept, one of the two detector concepts for the future International Linear Collider.…

Instrumentation and Detectors · Physics 2021-09-03 Fabricio Jimenez Morales

Micro-pattern gaseous detectors (MPGDs) are a promising readout technology for hadronic calorimeters (HCAL) thanks to their good space resolution, longevity and rate capability. We describe the development of a HCAL based on MPGDs for an…

The CMS Hadron Calorimeter in the barrel, endcap and forward regions is fully commissioned. Cosmic ray data were taken with and without magnetic field at the surface hall and after installation in the experimental hall, hundred meters…

Instrumentation and Detectors · Physics 2012-08-27 CMS Collaboration

CALICE collaboration is developing highly granular calorimeters suitable for individual reconstruction of particles in the jets using Particle Flow Algorithms. Such calorimeters should provide the best jet energy resolution at future high…

Instrumentation and Detectors · Physics 2018-02-05 Kostiantyn Shpak

TileCal is the hadronic calorimeter covering the most central region of the ATLAS experiment at the LHC. This sampling calorimeter uses iron plates as absorber and plastic scintillating tiles as the active material. A multi-faceted…

Instrumentation and Detectors · Physics 2012-12-18 Olof Lundberg

ALICE (A Large Ion Collider Experiment) at the LHC is designed for studies of nuclear matter at extreme temperatures and energy densities, so called Quark-Gluon Plasma (QGP). Two detectors for measurements of electromagnetic signals,…

High Energy Physics - Experiment · Physics 2020-04-22 D. Blau

The original dual-readout calorimeter prototype (DREAM), constructed two decades ago, has proven instrumental in advancing our understanding of calorimetry. It has facilitated a multitude of breakthroughs by leveraging signals from…

Instrumentation and Detectors · Physics 2024-08-29 N. Akchurin , J. Cash , J. Damgov , X. Delashaw , K. Lamichhane , M. Harris , M. Kelley , S. Kunori , H. Mergate-Cacace , T. Peltola , O. Schneider , J. Sewell

This study constructs a hybrid module with a multi-material collaborative detection architecture by integrating silicon pixel layers into the longitudinally segmented scintillating fiber sampling calorimeter module and optimizes the…

Instrumentation and Detectors · Physics 2025-09-30 Jia-Le Fei , Ao Yuan , Chang-Heng Huang , Liu-Pan An , Ji-Ke Wang

As a future Higgs or Z factory, construction of the circular electron positron collider(CEPC) has been proposed to precisely measure Higgs bosons. A particle flow-oriented electromagnetic calorimeter (ECAL) and a hadronic calorimeter…

Instrumentation and Detectors · Physics 2020-06-17 YZ. Niu

Calorimeters with a high granularity are a fundamental requirement of the Particle Flow paradigm. This paper focuses on the prototype of a hadron calorimeter with analog readout, consisting of thirty-eight scintillator layers alternating…

Instrumentation and Detectors · Physics 2014-06-17 C. Adloff , J. Blaha , J. -J. Blaising , C. Drancourt , A. Espargilière , R. Gaglione , N. Geffroy , Y. Karyotakis , J. Prast , G. Vouters , K. Francis , J. Repond , J. Schlereth , J. Smith , L. Xia , E. Baldolemar , J. Li , S. T. Park , M. Sosebee , A. P. White , J. Yu , T. Buanes , G. Eigen , Y. Mikami , N. K. Watson , G. Mavromanolakis , M. A. Thomson , D. R. Ward , W. Yan , D. Benchekroun , A. Hoummada , Y. Khoulaki , J. Apostolakis , A. Dotti , G. Folger , V. Ivantchenko , V. Uzhinskiy , M. Benyamna , C. Cârloganu , F. Fehr , P. Gay , S. Manen , L. Royer , G. C. Blazey , A. Dyshkant , J. G. R. Lima , V. Zutshi , J. -Y. Hostachy , L. Morin , U. Cornett , D. David , G. Falley , K. Gadow , P. Göttlicher , C. Günter , B. Hermberg , S. Karstensen , F. Krivan , A. -I. Lucaci-Timoce , S. Lu , B. Lutz , S. Morozov , V. Morgunov , M. Reinecke , F. Sefkow , P. Smirnov , M. Terwort , A. Vargas-Trevino , N. Feege , E. Garutti , I. Marchesinik , M. Ramilli , P. Eckert , T. Harion , A. Kaplan , H. -Ch. Schultz-Coulon , W. Shen , R. Stamen , B. Bilki , E. Norbeck , Y. Onel , G. W. Wilson , K. Kawagoe , P. D. Dauncey , A. -M. Magnan , V. Bartsch , M. Wing , F. Salvatore , E. Calvo Alamillo , M. -C. Fouz , J. Puerta-Pelayo , B. Bobchenko , M. Chadeeva , M. Danilov , A. Epifantsev , O. Markin , R. Mizuk , E. Novikov , V. Popov , V. Rusinov , E. Tarkovsky , N. Kirikova , V. Kozlov , P. Smirnov , Y. Soloviev , P. Buzhan , A. Ilyin , V. Kantserov , V. Kaplin , A. Karakash , E. Popova , V. Tikhomirov , C. Kiesling , K. Seidel , F. Simon , C. Soldner , M. Szalay , M. Tesar , L. Weuste , M. S. Amjad , J. Bonis , S. Callier , S. Conforti di Lorenzo , P. Cornebise , Ph. Doublet , F. Dulucq , J. Fleury , T. Frisson , N. van der Kolk , H. Li , G. Martin-Chassard , F. Richard , Ch. de la Taille , R. Pöschl , L. Raux , J. Rouëné , N. Seguin-Moreau , M. Anduze , V. Boudry , J-C. Brient , D. Jeans , P. Mora de Freitas , G. Musat , M. Reinhard , M. Ruan , H. Videau , B. Bulanek , J. Zacek , J. Cvach , P. Gallus , M. Havranek , M. Janata , J. Kvasnicka , D. Lednicky , M. Marcisovsky , I. Polak , J. Popule , L. Tomasek , M. Tomasek , P. Ruzicka , P. Sicho , J. Smolik , V. Vrba , J. Zalesak , B. Belhorma , H. Ghazlane , T. Takeshita , S. Uozumi , M. Götze , O. Hartbrich , J. Sauer , S. Weber , C. Zeitnitz

The goal of the T3B experiment is the measurement of the time structure of hadronic showers with nanosecond precision and high spatial resolution together with the CALICE hadron calorimeter prototypes, with a focus on the use of tungsten as…

Instrumentation and Detectors · Physics 2013-12-05 Frank Simon , Christian Soldner , Lars Weuste

A highly granular silicon-tungsten electromagnetic calorimeter (SiW-ECAL) is the reference design of the ECAL of the International Large Detector (ILD) concept, one of the two detector concepts for the detector(s) at the future…

Instrumentation and Detectors · Physics 2020-06-17 D. Breton , A. Irles , J. Jeglot , J. Maalmi , R. Pöschl , D. Zerwas

Detectors proposed for the International Linear Collider (ILC) incorporate a tungsten sampling calorimeter (`BeamCal') intended to reconstruct showers of electrons, positrons and photons that emerge from the interaction point of the…

The Particle Flow Analysis approach retained for the future ILC detectors requires high granularity and compact particle energy deposition. A Glass Resistive Plate Chamber based Semi-Digital calorimeter can offer both at a low price for the…

Instrumentation and Detectors · Physics 2019-08-13 Vincent Boudry

The Tile Calorimeter (TileCal) of the ATLAS experiment at the LHC is the central hadronic calorimeter designed for reconstruction of hadrons, jets, tau-particles and missing transverse energy. TileCal is a scintillator-steel sampling…

Instrumentation and Detectors · Physics 2017-09-04 Michaela Mlynarikova

We describe the design and performance the calorimeter systems used in the ECCE detector design to achieve the overall performance specifications cost-effectively with careful consideration of appropriate technical and schedule risks. The…

Instrumentation and Detectors · Physics 2023-08-09 F. Bock , N. Schmidt , P. K. Wang , N. Santiesteban , T. Horn , J. Huang , J. Lajoie , C. Munoz Camacho , J. K. Adkins , Y. Akiba , A. Albataineh , M. Amaryan , I. C. Arsene , C. Ayerbe Gayoso , J. Bae , X. Bai , M. D. Baker , M. Bashkanov , R. Bellwied , F. Benmokhtar , V. Berdnikov , J. C. Bernauer , W. Boeglin , M. Borysova , E. Brash , P. Brindza , W. J. Briscoe , M. Brooks , S. Bueltmann , M. H. S. Bukhari , A. Bylinkin , R. Capobianco , W. -C. Chang , Y. Cheon , K. Chen , K. -F. Chen , K. -Y. Cheng , M. Chiu , T. Chujo , Z. Citron , E. Cline , E. Cohen , T. Cormier , Y. Corrales Morales , C. Cotton , J. Crafts , C. Crawford , S. Creekmore , C. Cuevas , J. Cunningham , G. David , C. T. Dean , M. Demarteau , S. Diehl , N. Doshita , R. Dupre , J. M. Durham , R. Dzhygadlo , R. Ehlers , L. El Fassi , A. Emmert , R. Ent , C. Fanelli , R. Fatemi , S. Fegan , M. Finger , M. Finger , J. Frantz , M. Friedman , I. Friscic , D. Gangadharan , S. Gardner , K. Gates , F. Geurts , R. Gilman , D. Glazier , E. Glimos , Y. Goto , N. Grau , S. V. Greene , A. Q. Guo , L. Guo , S. K. Ha , J. Haggerty , T. Hayward , X. He , O. Hen , D. W. Higinbotham , M. Hoballah , A. Hoghmrtsyan , P. -h. J. Hsu , G. Huber , A. Hutson , K. Y. Hwang , C. E. Hyde , M. Inaba , T. Iwata , H. S. Jo , K. Joo , N. Kalantarians , G. Kalicy , K. Kawade , S. J. D. Kay , A. Kim , B. Kim , C. Kim , M. Kim , Y. Kim , Y. Kim , E. Kistenev , V. Klimenko , S. H. Ko , I. Korover , W. Korsch , G. Krintiras , S. Kuhn , C. -M. Kuo , T. Kutz , D. Lawrence , S. Lebedev , H. Lee , J. S. H. Lee , S. W. Lee , Y. -J. Lee , W. Li , W. B. Li , X. Li , X. Li , X. Li , X. Li , Y. T. Liang , S. Lim , C. -h. Lin , D. X. Lin , K. Liu , M. X. Liu , K. Livingston , N. Liyanage , W. J. Llope , C. Loizides , E. Long , R. -S. Lu , Z. Lu , W. Lynch , S. Mantry , D. Marchand , M. Marcisovsky , C. Markert , P. Markowitz , H. Marukyan , P. McGaughey , M. Mihovilovic , R. G. Milner , A. Milov , Y. Miyachi , A. Mkrtchyan , P. Monaghan , R. Montgomery , D. Morrison , A. Movsisyan , H. Mkrtchyan , A. Mkrtchyan , M. Murray , K. Nagai , J. Nagle , I. Nakagawa , C. Nattrass , D. Nguyen , S. Niccolai , R. Nouicer , G. Nukazuka , M. Nycz , V. A. Okorokov , S. Oresic , J. D. Osborn , C. O Shaughnessy , S. Paganis , Z. Papandreou , S. F. Pate , M. Patel , C. Paus , G. Penman , M. G. Perdekamp , D. V. Perepelitsa , H. Periera da Costa , K. Peters , W. Phelps , E. Piasetzky , C. Pinkenburg , I. Prochazka , T. Protzman , M. L. Purschke , J. Putschke , J. R. Pybus , R. Rajput-Ghoshal , J. Rasson , B. Raue , K. F. Read , K. Røed , R. Reed , J. Reinhold , E. L. Renner , J. Richards , C. Riedl , T. Rinn , J. Roche , G. M. Roland , G. Ron , M. Rosati , C. Royon , J. Ryu , S. Salur , R. Santos , M. Sarsour , J. Schambach , A. Schmidt , C. Schwarz , J. Schwiening , R. Seidl , A. Sickles , P. Simmerling , S. Sirca , D. Sharma , Z. Shi , T. -A. Shibata , C. -W. Shih , S. Shimizu , U. Shrestha , K. Slifer , K. Smith , D. Sokhan , R. Soltz , W. Sondheim , J. Song , J. Song , I. I. Strakovsky , P. Steinberg , P. Stepanov , J. Stevens , J. Strube , P. Sun , X. Sun , K. Suresh , V. Tadevosyan , W. -C. Tang , S. Tapia Araya , S. Tarafdar , L. Teodorescu , D. Thomas , A. Timmins , L. Tomasek , N. Trotta , R. Trotta , T. S. Tveter , E. Umaka , A. Usman , H. W. van Hecke , C. Van Hulse , J. Velkovska , E. Voutier , P. K. Wang , Q. Wang , Y. Wang , Y. Wang , D. P. Watts , N. Wickramaarachchi , L. Weinstein , M. Williams , C. -P. Wong , L. Wood , M. H. Wood , C. Woody , B. Wyslouch , Z. Xiao , Y. Yamazaki , Y. Yang , Z. Ye , H. D. Yoo , M. Yurov , N. Zachariou , W. A. Zajc , W. Zha , J. -L. Zhang , J. -X. Zhang , Y. Zhang , Y. -X. Zhao , X. Zheng , P. Zhuang

The foreseen upgrade of the LHC to its high luminosity phase (HL-LHC), will maximize the physics potential of the facility. The upgrade is expected to increase the instantaneous luminosity by a factor of 5 and deliver an integrated…

Instrumentation and Detectors · Physics 2018-12-19 Timo Peltola