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Analysis of the CMS data and the simulation prediction based on these results indicate that the performance of the current scintillators in the CMS Hadron Endcap Calorimeter (HE) tiles will degrade dramatically in the High Luminosity LHC…

Instrumentation and Detectors · Physics 2013-08-30 Yasar Onel , David Winn

We report on the design and performance of the electromagnetic calorimeter timing readout system (EMTiming) for the Collider Detector at Fermilab (CDF). The system will be used in searches for rare events with high energy photons to verify…

Instrumentation and Detectors · Physics 2008-11-26 M. Goncharov , T. Kamon , V. Khotilovich , V. Krutelyov , S. W. Lee , D. Toback , P. Wagner , H. Frisch , H. Sanders , M. Cordelli , F. Happacher , S. Miscetti , R. Wagner

We present a description of the CMS central hadron calorimeter. We describe the production of the 1996 CMS hadron testbeam module. We show the results of the quality control tests of the testbeam module. We present some results of the 1995…

High Energy Physics - Experiment · Physics 2009-11-07 Howard S. Budd

The Compact Muon Solenoid (CMS) detector is a general-purpose experimental setup at the Large Hadron Collider (LHC) at CERN to investigate the production of new particles in the proton-proton collisions at a centre of mass energy 13 TeV.…

Instrumentation and Detectors · Physics 2022-10-13 Vyacheslav Klyukhin

We present results on the performance of the first prototype of the CASTOR quartz-tungsten sampling calorimeter, to be installed in the very forward region of the CMS experiment at the LHC. This study includes GEANT Monte Carlo simulations…

Instrumentation and Detectors · Physics 2008-11-26 X. Aslanoglou , A. Cyz , N. Davis , D. d'Enterria , E. Gladysz-Dziadus , C. Kalfas , Y. Musienko , A. Kuznetsov , A. D. Panagiotou

The upgrade of the CMS experiment for the high luminosity operation of the LHC comprises the replacement of the current endcap calorimeter by a high granularity sampling calorimeter (HGCAL). The electromagnetic section of the HGCAL is based…

Instrumentation and Detectors · Physics 2023-05-30 B. Acar , G. Adamov , C. Adloff , S. Afanasiev , N. Akchurin , B. Akgün , M. Alhusseini , J. Alison , J. P. Figueiredo de sa Sousa de Almeida , P. G. Dias de Almeida , A. Alpana , M. Alyari , I. Andreev , U. Aras , P. Aspell , I. O. Atakisi , O. Bach , A. Baden , G. Bakas , A. Bakshi , S. Banerjee , P. DeBarbaro , P. Bargassa , D. Barney , F. Beaudette , F. Beaujean , E. Becheva , A. Becker , P. Behera , A. Belloni , T. Bergauer , M. El Berni , M. Besancon , S. Bhattacharya , S. Bhattacharya , D. Bhowmik , B. Bilki , S. Bilokin , G. C. Blazey , F. Blekman , P. Bloch , A. Bodek , M. Bonanomi , J. Bonis , A. Bonnemaison , S. Bonomally , J. Borg , F. Bouyjou , N. Bower , D. Braga , L. Brennan , E. Brianne , E. Brondolin , P. Bryant , E. Buhmann , P. Buhmann , A. Butler-Nalin , O. Bychkova , S. Callier , D. Calvet , K. Canderan , K. Cankocak , X. Cao , A. Cappati , B. Caraway , S. Caregari , C. Carty , A. Cauchois , L. Ceard , D. S. Cerci , S. Cerci , G. Cerminara , M. Chadeeva , N. Charitonidis , R. Chatterjee , J. A. Chen , Y. M. Chen , H. J. Cheng , K. Y. Cheng , H. Cheung , D. Chokheli , M. Cipriani , D. Čoko , F. Couderc , E. Cuba , M. Danilov , D. Dannheim , W. Daoud , I. Das , P. Dauncey , G. Davies , O. Davignon , E. Day , P. Debbins , M. M. Defranchis , E. Delagnes , Z. Demiragli , U. Demirbas , G. Derylo , D. Diaz , L. Diehl , P. Dinaucourt , G. G. Dincer , J. Dittmann , M. Dragicevic , S. Dugad , F. Dulucq , I. Dumanoglu , M. Dünser , S. Dutta , V. Dutta , T. K. Edberg , F. Elias , L. Emberger , S. C. Eno , Yu. Ershov , S. Extier , F. Fahim , C. Fallon , K. Sarbandi Fard , G. Fedi , L. Ferragina , L. Forthomme , E. Frahm , G. Franzoni , J. Freeman , T. French , K. Gadow , P. Gandhi , S. Ganjour , X. Gao , M. T. Ramos Garcia , A. Garcia-Bellido , E. Garutti , F. Gastaldi , D. Gastler , Z. Gecse , A. Germer , H. Gerwig , O. Gevin , S. Ghosh , A. Gilbert , W. Gilbert , K. Gill , C. Gingu , S. Gninenko , A. Golunov , I. Golutvin , B. Gonultas , N. Gorbounov , P. Göttlicher , L. Gouskos , C. Graf , A. B. Gray , C. Grieco , S. Gr\"önroos , Y. Gu , F. Guilloux , E. Gurpinar Guler , Y. Guler , E. Gülmez , J. Guo , H. Gutti , A. Hakimi , M. Hammer , O. Hartbrich , H. M. Hassanshahi , K. Hatakeyama , E. Hazen , A. Heering , V. Hegde , U. Heintz , D. Heuchel , N. Hinton , J. Hirschauer , J. Hoff , W. S. Hou , X. Hou , H. Hua , S. Huck , A. Hussain , J. Incandela , A. Irles , A. Irshad , C. Isik , S. Jain , J. Jaroslavceva , H. R. Jheng , U. Joshi , K. Kaadze , V. Kachanov , L. Kalipoliti , A. Kaminskiy , A. R. Kanuganti , Y. W. Kao , A. Kapoor , O. Kara , A. Karneyeu , O. Kałuzińska , M. Kaya , O. Kaya , Y. Kazhykharim , F. A. Khan , A. Khukhunaishvili , J. Kieseler , M. Kilpatrick , S. Kim , K. Koetz , T. Kolberg , M. Komm , O. K. Köseyan , V. Kraus , M. Krawczyk , K. Kristiansen , A. Kristić , M. Krohn , B. Kronheim , K. Krüger , S. Kulis , M. Kumar , S. Kunori , C. M. Kuo , V. Kuryatkov , J. Kvasnicka , S. Kyre , Y. Lai , K. Lamichhane , G. Landsberg , C. Lange , J. Langford , S. Laurien , M. Y. Lee , S. W. Lee , A. G. Stahl Leiton , A. Levin , A. Li , J. H. Li , Y. Y. Li , Z. Liang , H. Liao , Z. Lin , D. Lincoln , L. Linssen , R. Lipton , G. Liu , Y. Liu , A. Lobanov , V. Lohezic , D. Lomidze , R. S. Lu , S. Lu , M. Lupi , I. Lysova , A. -M. Magnan , F. Magniette , A. Mahjoub , S. Martens , M. Matysek , B. Meier , A. Malakhov , S. Mallios , I. Mandjavize , M. Mannelli , J. Mans , A. Marchioro , A. Martelli , G. Martinez , P. Masterson , M. Matthewman , S. N. Mayekar , A. David , S. Coco , B. Meng , A . Menkel , A. Mestvirishvili , G. Milella , I. Mirza , S. Moccia , G. B. Mohanty , F. Monti , F. W. Moortgat , I. Morrissey , J. Motta , S. Murthy , J. Musić , Y. Musienko , S. Nabili , M. Nguyen , A. Nikitenko , D. Noonan , D. Noonan , M. Noy , K. Nurdan , M. Wulansatiti Nursanto , C. Ochando , N. Odell , H. Okawa , Y. Onel , W. Ortez , J. Ozegović , S. Ozkorucuklu , E. Paganis , C. A. Palmer , S. Pandey , F. Pantaleo , C. Papageorgakis , I. Papakrivopoulos , M. Paranjpe , J. Parshook , N. Pastika , M. Paulini , T. Peitzmann , T. Peltola , N. Peng , A. Buchot Perraguin , P. Petiot , T. Pierre-Emile , M. Vicente Barreto Pinto , E. Popova , R. Pöschl , H. Prosper , M. Prvan , I. Puljak , S. R. Qasim , H. Qu , T. Quast , R. Quinn , M. Quinnan , A. Rane , K. K. Rao , K. Rapacz , L. Raux , W. Redjeb , M. Reinecke , M. Revering , F. Richard , A. Roberts , A. M. Sanchez , J. Rohlf , J. Rolph , T. Romanteau , M. Rosado , A. Rose , M. Rovere , A. Roy , P. Rubinov , R. Rusack , V. Rusinov , V. Ryjov , O. M. Sahin , R. Salerno , R. Saradhy , T. Sarkar , M. A. Sarkisla , J. B. Sauvan , I. Schmidt , M. Schmitt , S. Schuwalow , E. Scott , C. Seez , F. Sefkow , D. Selivanova , S. Sharma , M. Shelake , A. Shenai , R. Shukla , E. Sicking , M. De , P. Silva , P. Simkina , F. Simon , A. E. Simsek , Y. Sirois , V. Smirnov , T. J. Sobering , E. Spencer , N. Srimanobhas , A. Steen , J. Strait , N. Strobbe , X. F. Su , Y. Sudo , C. Mantilla Suarez , E. Sukhov , L. Sulak , L. Sun , P. Suryadevara , C. Syal , C. de La Taille , B. Tali , C. L. Tan , J. Tao , A. Tarabini , T. Tatli , R. Thaus , R. D. Taylor , S. Tekten , A. Thiebault , D. Thienpont , C. Tiley , E. Tiras , M. Titov , D. Tlisov , U. G. Tok , A. Kayis , J. Troska , L. S. Tsai , Z. Tsamalaidze , G. Tsipolitis , A. Tsirou , S. Undleeb , D. Urbanski , E. Uslan , V. Ustinov , A. Uzunian , J. Varela , M. Velasco , E. Vernazza , O. Viazlo , P. Vichoudis , T. Virdee , E. Voirin , M. Vojinovi\c , M. Vojinovic , A. Wade , C. Wang , C. C. Wang , D. Wang , F. Wang , X. Wang , X. Wang , Z. Wang , M. Wayne , S. N. Webb , A. Whitbeck , R. Wickwire , J. S. Wilson , H. Y. Wu , L. Wu , M. Xiao , J. Yang , C. H Yeh , R. Yohay , D. Yu , S. S. Yu , C. Yuan , Y. Miao , F. Yumiceva , I. Yusuff , A. Zabi , A. Zacharopoulou , N. Zamiatin , A. Zarubin , P. Zehetner , D. Zerwas , H. Zhang , J. Zhang , Y. Zhang , Z. Zhang , X. Zhao

The capabilities of the CMS detector at the LHC will be described for measuring high-pT hadrons, photons and jets in heavy ion collisions. Detailed simulations of various studies planned with the CMS apparatus, including charged particle…

Nuclear Experiment · Physics 2019-08-13 Gábor I. Veres

A template fitting technique for reconstructing the amplitude of signals produced by the lead tungstate crystals of the CMS electromagnetic calorimeter is described. This novel approach is designed to suppress the increased out-of-time…

Instrumentation and Detectors · Physics 2020-10-05 CMS Collaboration

The calorimeter system of LHCb is subdivided into four sub-detectors which ensure its longitudinal segmentation: a Scintillator Pad Detector (SPD) followed by a Preshower (PS) and then an electromagnetic (ECAL) an hadronic (HCAL)…

Instrumentation and Detectors · Physics 2019-08-13 Pascal Perret

A novel design for a silicon-tungsten electromagnetic calorimeter is described, based on Monolithic Active Pixel Sensors (MAPS). A test sensor with a pixel size of 50x50 um2 has been fabricated in July 2007. The simulation of the physical…

In order to get ready for physics at the LHC, the CMS experiment has to be set up for data taking. The data have to be well understood before new physics can be investigated. On the other hand, there are standard processes, well known from…

Instrumentation and Detectors · Physics 2016-11-09 V. Drollinger

We present a new publicly available dataset that contains simulated data of a novel calorimeter to be installed at the CERN Large Hadron Collider. This detector will have more than six-million channels with each channel capable of position,…

High Energy Physics - Experiment · Physics 2023-09-14 Roger Rusack , Bhargav Joshi , Alpana Alpana , Seema Sharma , Thomas Vadnais

The performance of the electromagnetic calorimeter of the HERMES experiment is described. The calorimeter consists of 840 radiation resistant F101 lead-glass counters. The response to positrons up to 27.5 GeV, the comparison between the…

High Energy Physics - Experiment · Physics 2015-06-25 H. Avakian

The very-forward energy production in hadron collisions is of paramount importance for the understanding of ultra-high energy cosmic ray air showers. The CASTOR calorimeter of CMS is located at $-6.6 < \eta < -5.2$ in the phase-space where…

High Energy Physics - Experiment · Physics 2019-05-22 Sebastian Baur

Two different technologies are considered for the Beam Calorimeters of the ILC detector. Simulation studies of the performance have been done for a diamond-tungsten sandwich calorimeter and for a homogeneous heavy element crystal…

Instrumentation and Detectors · Physics 2007-05-23 R. Dollan , Ch. Grah , E. Kuznetsova , W. Lange , W. Lohmann , A. Stahl , K. Afanaciev , V. Drugakov , I. Emeliantchik

The CMS experiment is a multi-purpose detector successfully operated at the LHC where predominantly pp collisions take place at various centre-of-mass energies up to sqrt(s)=8 TeV so far. Several weeks per year also heavy-ion collisions…

High Energy Physics - Experiment · Physics 2014-08-19 Lars Sonnenschein

The HL-LHC and the corresponding detector upgrades for the CMS experiment will present extreme challenges for the full simulation. In particular, increased precision in models of physics processes may be required for accurate reproduction…

Computational Physics · Physics 2020-11-19 Kevin Pedro

A brief summary of the hadronic calorimeter calibration systems and performance results, in the ATLAS detector at the LHC is given.

Instrumentation and Detectors · Physics 2019-08-13 Chris Meyer

Commissioning studies of the CMS hadron calorimeter have identified sporadic uncharacteristic noise and a small number of malfunctioning calorimeter channels. Algorithms have been developed to identify and address these problems in the…

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

The CMS experiment at the LHC has started data taking in Run 3 at a $\mathrm{pp}$ collision energy of $13.6~\mathrm{TeV}$. In preparation for Run 3, detector systems, such as Pixel Tracker, HCAL and CSC, have been upgraded due to…

High Energy Physics - Experiment · Physics 2023-09-07 Srećko Morović