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A prototype of a new type of calorimeter has been designed and constructed, based on a silicon-tungsten sampling design using pixel sensors with digital readout. It makes use of the Alpide MAPS sensor developed for the ALICE ITS upgrade. A…

Crystal electromagnetic calorimeters (ECALs) are essential for high-precision measurements of electrons and photons in particle physics experiments. However, the conventional design, in which long crystal bars point radially toward the…

Instrumentation and Detectors · Physics 2026-02-26 Weizheng Song , Yang Zhang , Shengsen Sun , Fangyi Guo , Yuanzhan Wang , Linghui Wu , Jie Guo , Shaojing Hou , Yong Liu , Quan Ji , Jinfan Chang , Yifang Wang

The Belle II experiment is presently in phase-2 operation at the SuperKEKB electron-positron collider in KEK (Tsukuba, Japan). The detector is an upgrade of the Belle experiment at the KEKB collider and it is optimized for the study of rare…

Instrumentation and Detectors · Physics 2018-07-04 V. Izzo , A. Aloisio , F. Ameli , A. Anastasio , P. Branchini , F. Di Capua , R. Giordano , A. Kuzmin , K. Miyabayashi , I. Nakamura , M. Nakao , G. Tortone , S. Uehara

We report on the development of an GRPCs (Glass Resistive Plate chambers) Semi- Digital hadron calorimeter for the future International Linear Collider (ILC).Two types of GRPCs (small and 1m2) were tested in PS beam at CERN. Detector…

Instrumentation and Detectors · Physics 2010-08-24 Khaled Belkadhi

LumiCal is a sampling electromagnetic calorimeter designed for the precise measurement of integrated luminosity in electron positron linear collider experiments. The present report contains a description and results of the first beam test…

Instrumentation and Detectors · Physics 2019-08-13 Oleksandr Borysov

The High Luminosity Large Hadron Collider (HL-LHC) will have a peak luminosity of $5\times10^{34} $cm$^{-2} $\,s$^{-1}$, five times higher than the design luminosity of the LHC. The hadronic ATLAS Tile Calorimeter TileCal) is a sampling…

Instrumentation and Detectors · Physics 2020-10-29 Eduardo Valdes Santurio

The ILD Si-W ECAL is a sampling calorimeter with tungsten absorber and highly segmented silicon layers for the International Large Detector (ILD), one of the two detector concepts for the International Linear Collider. SKIROC2 is an ASIC…

This document presents the technical layout and the envisaged performance of the Electromagnetic Calorimeter (EMC) for the PANDA target spectrometer. The EMC has been designed to meet the physics goals of the PANDA experiment, which is…

Instrumentation and Detectors · Physics 2019-08-17 PANDA Collaboration , W. Erni , I. Keshelashvili , B. Krusche , M. Steinacher , Y. Heng , Z. Liu , H. Liu , X. Shen , O. Wang , H. Xu , J. Becker , F. Feldbauer , F. -H. Heinsius , T. Held , H. Koch , B. Kopf , M. Pelizaeus , T. Schroeder , M. Steinke , U. Wiedner , J. Zhong , A. Bianconi , M. Bragadireanu , D. Pantea , A. Tudorache , V. Tudorache , M. De Napoli , F. Giacoppo , G. Raciti , E. Rapisarda , C. Sfienti , E. Bialkowski , A. Budzanowski , B. Czech , M. Kistryn , S. Kliczewski , A. Kozela , P. Kulessa , K. Pysz , W. Schaefer , R. Siudak , A. Szczurek , W. Czy. zycki , M. Domagala , M. Hawryluk , E. Lisowski , F. Lisowski , L. Wojnar , D. Gil , P. Hawranek , B. Kamys , St. Kistryn , K. Korcyl , W. Krzemien , A. Magiera , P. Moskal , Z. Rudy , P. Salabura , J. Smyrski , A. Wronska , M. Al-Turany , I. Augustin , H. Deppe , H. Flemming , J. Gerl , K. Goetzen , R. Hohler , D. Lehmann , B. Lewandowski , J. Luehning , F. Maas , D. Mishra , H. Orth , K. Peters , T. Saito , G. Schepers , C. J. Schmidt , L. Schmitt , C. Schwarz , B. Voss , P. Wieczorek , A. Wilms , K. -T. Brinkmann , H. Freiesleben , R. Jaekel , R. Kliemt , T. Wuerschig , H. -G. Zaunick , V. M. Abazov , G. Alexeev , A. Arefiev , V. I. Astakhov , M. Yu. Barabanov , B. V. Batyunya , Yu. I. Davydov , V. Kh. Dodokhov , A. A. Efremov , A. G. Fedunov , A. A. Feshchenko , A. S. Galoyan , S. Grigoryan , A. Karmokov , E. K. Koshurnikov , V. Ch. Kudaev , V. I. Lobanov , Yu. Yu. Lobanov , A. F. Makarov , L. V. Malinina , V. L. Malyshev , G. A. Mustafaev , A. Olshevski , M. A. Pasyuk , E. A. Perevalova , A. A. Piskun , T. A. Pocheptsov , G. Pontecorvo , V. K. Rodionov , Yu. N. Rogov , R. A. Salmin , A. G. Samartsev , M. G. Sapozhnikov , A. Shabratova , G. S. Shabratova , A. N. Skachkova , N. B. Skachkov , E. A. Strokovsky , M. K. Suleimanov , R. Sh. Teshev , V. V. Tokmenin , V. V. Uzhinsky , A. S. Vodopianov , S. A. Zaporozhets , N. I. Zhuravlev , A. G. Zorin , D. Branford , K. Foehl , D. Glazier , D. Watts , P. Woods , W. Eyrich , A. Lehmann , A. Teufel , S. Dobbs , Z. Metreveli , K. Seth , B. Tann , A. Tomaradze , D. Bettoni , V. Carassiti , A. Cecchi , P. Dalpiaz , E. Fioravanti , I. Garzia , M. Negrini , M. Savri`e , G. Stancari , B. Dulach , P. Gianotti , C. Guaraldo , V. Lucherini , E. Pace , A. Bersani , M. Macri , M. Marinelli , R. F. Parodi , I. Brodski , W. Doering , P. Drexler , M. Dueren , Z. Gagyi-Palffy , A. Hayrapetyan , M. Kotulla , W. Kuehn , S. Lange , M. Liu , V. Metag , M. Nanova , R. Novotny , C. Salz , J. Schneider , P. Schoenmeier , R. Schubert , S. Spataro , H. Stenzel , C. Strackbein , M. Thiel , U. Thoering , S. Yang , T. Clarkson , E. Cowie , E. Downie , G. Hill , M. Hoek , D. Ireland , R. Kaiser , T. Keri , I. Lehmann , K. Livingston , S. Lumsden , D. MacGregor , B. McKinnon , M. Murray , D. Protopopescu , G. Rosner , B. Seitz , G. Yang , M. Babai , A. K. Biegun , A. Bubak , E. Guliyev , V. S. Jothi , M. Kavatsyuk , H. Loehner , J. Messchendorp , H. Smit , J. C. van der Weele , F. Garcia , D. -O. Riska , M. Buescher , R. Dosdall , R. Dzhygadlo , A. Gillitzer , D. Grunwald , V. Jha , G. Kemmerling , H. Kleines , A. Lehrach , R. Maier , M. Mertens , H. Ohm , D. Prasuhn , T. Randriamalala , J. Ritman , M. Roeder , T. Stockmanns , P. Wintz , P. Wuestner , J. Kisiel , S. Li , Z. Li , Z. Sun , H. Xu , S. Fissum , K. Hansen , L. Isaksson , M. Lundin , B. Schroeder , P. Achenbach , M. C. Mora Espi , J. Pochodzalla , S. Sanchez , A. Sanchez-Lorente , V. I. Dormenev , A. A. Fedorov , M. V. Korzhik , O. V. Missevitch , V. Balanutsa , V. Chernetsky , A. Demekhin , A. Dolgolenko , P. Fedorets , A. Gerasimov , V. Goryachev , A. Boukharov , O. Malyshev , I. Marishev , A. Semenov , C. Hoeppner , B. Ketzer , I. Konorov , A. Mann , S. Neubert , S. Paul , Q. Weitzel , A. Khoukaz , T. Rausmann , A. Taeschner , J. Wessels , R. Varma , E. Baldin , K. Kotov , S. Peleganchuk , Yu. Tikhonov , J. Boucher , T. Hennino , R. Kunne , S. Ong , J. Pouthas , B. Ramstein , P. Rosier , M. Sudol , J. Van de Wiele , T. Zerguerras , K. Dmowski , R. Korzeniewski , D. Przemyslaw , B. Slowinski , G. Boca , A. Braghieri , S. Costanza , A. Fontana , P. Genova , L. Lavezzi , P. Montagna , A. Rotondi , N. I. Belikov , A. M. Davidenko , A. A. Derevschikov , Y. M. Goncharenko , V. N. Grishin , V. A. Kachanov , D. A. Konstantinov , V. A. Kormilitsin , V. I. Kravtsov , Y. A. Matulenko , Y. M. Melnik , A. P. Meschanin , N. G. Minaev , V. V. Mochalov , D. A. Morozov , L. V. Nogach , S. B. Nurushev , A. V. Ryazantsev , P. A. Semenov , L. F. Soloviev , A. V. Uzunian , A. N. Vasiliev , A. E. Yakutin , T. Baeck , B. Cederwall , C. Bargholtz , L. Geren , P. E. Tegner , S. Belostotski , G. Gavrilov , A. Itzotov , A. Kisselev , P. Kravchenko , S. Manaenkov , O. Miklukho , Y. Naryshkin , D. Veretennikov , V. Vikhrov , A. Zhadanov , L. Fava , D. Panzieri , D. Alberto , A. Amoroso , E. Botta , T. Bressani , S. Bufalino , M. P. Bussa , L. Busso , F. De Mori , M. Destefanis , L. Ferrero , A. Grasso , M. Greco , T. Kugathasan , M. Maggiora , S. Marcello , G. Serbanut , S. Sosio , R. Bertini , D. Calvo , S. Coli , P. De Remigis , A. Feliciello , A. Filippi , G. Giraudo , G. Mazza , A. Rivetti , K. Szymanska , F. Tosello , R. Wheadon , O. Morra , M. Agnello , F. Iazzi , K. Szymanska , R. Birsa , F. Bradamante , A. Bressan , A. Martin , H. Clement , C. Ekstroem , H. Calen , S. Grape , B. Hoeistad , T. Johansson , A. Kupsc , P. Marciniewski , E. Thome , J. Zlomanczuk , J. Diaz , A. Ortiz , S. Borsuk , A. Chlopik , Z. Guzik , J. Kopec , T. Kozlowski , D. Melnychuk , M. Plominski , J. Szewinski , K. Traczyk , B. Zwieglinski , P. Buehler , A. Gruber , P. Kienle , J. Marton , E. Widmann , J. Zmeskal

Collider detectors have taken advantage of the resolution and accuracy of silicon detectors for at least four decades. Future colliders will need large areas of silicon sensors for low mass trackers and sampling calorimetry. Monolithic…

The status of the prototype readout boards for the CALICE electromagnetic calorimeter is presented. Results on linearity, noise, and minimum ionising signals, both from a radiactive source and cosmic rays, are shown.

High Energy Physics - Experiment · Physics 2007-05-23 P. D. Dauncey

Shashlyk-type electromagnetic calorimeter (ECal) of the Multi-Purpose Detector at heavy-ion NICA collider is optimized to provide precise spatial and energy measurements for photons and electrons in the energy range from about 40 MeV to 2-3…

Instrumentation and Detectors · Physics 2020-06-24 A. Yu. Semenov , I. A. Semenova , M. Bhattacharjee , A. Durum , Yu. Krechetov , V. Kulikov , I. Mamonov , M. Martemianov

The CALICE collaboration has constructed a highly granular hadronic calorimeter based on small scintillator tiles read out with silicon photomultipliers. With this detector, data was taken at CERN and at Fermilab. The high granularity of…

Instrumentation and Detectors · Physics 2019-08-13 Frank Simon

This report describes the physics potential and experiments at a future multi-TeV e+e- collider based on the Compact Linear Collider (CLIC) technology. The physics scenarios considered include precision measurements of known quantities as…

Instrumentation and Detectors · Physics 2012-04-22 Lucie Linssen , Akiya Miyamoto , Marcel Stanitzki , Harry Weerts

The Tile Calorimeter (TileCal) is a sampling hadronic calorimeter covering the central region of the ATLAS experiment. TileCal uses steel as absorber and plastic scintillators as active medium. The scintillators are read-out by the…

Instrumentation and Detectors · Physics 2021-05-20 Merve Nazlim Agaras

The operation and general performance of the CMS electromagnetic calorimeter using cosmic-ray muons are described. These muons were recorded after the closure of the CMS detector in late 2008. The calorimeter is made of lead tungstate…

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

Control of thermal emission is important in a number of applications from thermal energy harvesting and management and sensing of gas and chemical to thermal camouflage. Semiconductor-based devices can be engineered to enable electrical…

Applied Physics · Physics 2025-11-25 Sid Assawaworrarit , Alex Song , Shanhui Fan

Within the CALICE collaboration, several concepts for the hadronic calorimeter of a future linear collider detector are studied. After having demonstrated the capabilities of the measurement methods in "physics prototypes", the focus now…

Instrumentation and Detectors · Physics 2019-04-26 Christian Graf

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 Analog Hadron Calorimeter (AHCAL) concept developed by the CALICE collaboration is a highly granular sampling calorimeter with \SI{3x3}{\square\centi\meter} plastic scintillator tiles individually read out by silicon photomultipliers…

Instrumentation and Detectors · Physics 2021-05-19 Lorenz Emberger

A preliminary design of the PEP-N electromagnetic calorimeter is given. The spatial,energy and time resolutions achievable using a KLOE type electromagnetic calorimeter are presented.

High Energy Physics - Experiment · Physics 2014-11-17 P. Patteri