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Related papers: Fiber R and D for the CMS HCAL

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The CALICE analog HCAL is a highly granular calorimeter, proposed for the International Linear Collider. It is based on scintillator tiles, read out by silicon photomultipliers (SiPMs). The effects of gaps between the calorimeter tiles, as…

Instrumentation and Detectors · Physics 2010-06-21 Felix Sefkow , Angela Lucaci-Timoce

Digital Hadronic Calorimeters (DHCAL) were suggested for future Colliders as part of the particle-flow concept. Though studied mainly with Resistive Plate Chambers (RPC), studies focusing on Micro-Pattern Gaseous Detector (MPGD)-based…

As part of its HL-LHC upgrade program, CMS is developing a High Granularity Calorimeter (HGCAL) to replace the existing endcap calorimeters. The HGCAL will be realised as a sampling calorimeter, including an electromagnetic compartment…

Instrumentation and Detectors · Physics 2018-03-14 Thorben Quast

An analog hadron calorimeter (AHCAL) prototype of 5.3 nuclear interaction lengths thickness has been designed and constructed by members of the CALICE Collaboration. The AHCAL prototype consists of a 38-layer sandwich structure of steel…

Instrumentation and Detectors · Physics 2010-07-20 Shaojun Lu

A novel hadron calorimeter is being developed for future lepton colliding beam detectors. The calorimeter is optimized for the application of Particle Flow Algorithms (PFAs) to the measurement of hadronic jets and features a very finely…

A novel hadron calorimeter is being developed for future lepton colliding beam detectors. The calorimeter is optimized for the application of Particle Flow Algorithms (PFAs) to the measurement of hadronic jets and features a very finely…

The basic prototype of a tile hadron calorimeter (HCAL) for the International Linear Collider (ILC) has been realised and extensively tested. A major aspect of the proposed concept is the improvement of the jet energy resolution by…

Instrumentation and Detectors · Physics 2016-10-10 Aliakbar Ebrahimi

Glass RPC detectors are an attractive candidate for the active part of a highly granular digital hadron calorimeter (DHCAL) at the ILC. A numerical study, based on the GEANT3 simulation package, of the performance of such a calorimeter is…

Instrumentation and Detectors · Physics 2007-05-23 A. Ghezzi , T. Tabarelli de Fatis , G. Tinti , M. Piccolo

The Tile Calorimeter (TileCal) is the hadronic calorimeter covering the most central region of the ATLAS experiment at the LHC. It is a key detector for the measurement of hadrons, jets, tau leptons and missing transverse energy. The…

Instrumentation and Detectors · Physics 2013-05-03 Bernardo Sotto-Maior Peralva

The Analogue Hadron Calorimeter (AHCAL) developed by the CALICE collaboration is a scalable engineering prototype for a Linear Collider detector. It is a sampling calorimeter of steel absorber plates and plastic scintillator tiles read out…

Instrumentation and Detectors · Physics 2019-05-22 Felix Sefkow , Frank Simon

In special tests, the active layers of the CALICE Digital Hadron Calorimeter prototype, the DHCAL, were exposed to low energy particle beams, without being interleaved by absorber plates. The thickness of each layer corresponded…

The ATLAS Tile Calorimeter (TileCal) is the central section of the hadronic calorimeter of the ATLAS experiment at LHC. This sampling calorimeter uses steel plates as absorber and scintillating tiles as active medium. The light produced by…

Instrumentation and Detectors · Physics 2019-09-04 Marija Marjanovic

High performance calorimetry conducted at future hadron colliders, such as the FCC-hh, poses a significant challenge for applying current detector technologies due to unprecedented beam luminosities and radiation fields. Solutions include…

The CMS hadron Calorimeter is made of alternating layers of scintillating tiles and metals, such as brass or iron. The original photo detectors were hybrid units with a single accelerating gap called Hybrid Photo Diodes (HPD). Scintillating…

Instrumentation and Detectors · Physics 2018-06-27 R A Shukla , V G Achanta , P D Barbaro , S R Dugad , A Heering , S K Gupta , I Mirza , S S Prabhu , P Rumerio

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 2015-06-22 Gérald Grenier

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

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

In preparation of the operation of the CMS electromagnetic calorimeter (ECAL) barrel at the High Luminosity Large Hadron Collider (HL-LHC) the entire on-detector electronics will be replaced. The new readout electronics comprises 12240 very…

We review the status and plans of the Digital Hadron Calorimeter with Resistive Plate Chambers project.

Instrumentation and Detectors · Physics 2010-05-05 Jose Repond

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