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A front-end readout system with a large dynamic range is required for the high-granularity crystal electromagnetic calorimeter (ECAL) at future Higgs factories. A new commercially available ASIC, MPT2321, which offers a significantly large…

Instrumentation and Detectors · Physics 2025-05-23 Baohua Qi , Yong Liu , Huangchao Shi , Danqi Wang , Zhiyu Zhao , Hongbo Zhu

The High Luminosity LHC (HL-LHC) will integrate 10 times more luminosity than the LHC, posing significant challenges for radiation tolerance and event pileup on detectors, especially for forward calorimetry, and hallmarks the issue for…

Instrumentation and Detectors · Physics 2018-02-18 Arabella Martelli

We describe the electromagnetic calorimeter built for the GRAAL apparatus at the ESRF. Its monitoring system is presented in detail. Results from tests and the performance obtained during the first GRAAL experiments are given. The energy…

A new design of a detector plane of sub-millimetre thickness for an electromagnetic sampling calorimeter is presented. It is intended to be used in the luminometers LumiCal and BeamCal in future linear $e^+e^-$ collider experiments. The…

A silicon-tungsten (Si-W) sampling calorimeter, consisting of 19 alternate layers of silicon pad detectors (individual pad area of 1~cm$^2$) and tungsten absorbers (each of one radiation length), has been constructed for measurement of…

The scintillator-strip electromagnetic calorimeter (ScECAL) is one of the calorimeter technic for the ILC. To achieve the fine granularity from the strip-segmented layers the strips in odd layers are orthogonal with respect to those in the…

The Mu2e experiment at Fermilab will search for the charged lepton flavor violating process of neutrino-less $\mu \to e$ coherent conversion in the field of an aluminum nucleus. Mu2e will reach a single event sensitivity of about $2.5\cdot…

The MAPS prototype of the proposed ALICE Forward Calorimeter (FoCal) is the highest granularity electromagnetic calorimeter, with 39 million pixels of $30 \times 30 \mu$m$^{2}$. Particle showers can be studied with unprecedented detail with…

Instrumentation and Detectors · Physics 2018-07-01 Naomi van der Kolk

In the ILD detector, HCAL is inside the coil. The HCAL is about 5 interaction length thick, and ECAL is about 1 interaction length thick. For example, an eighty GeV hadron, it is only 95% energy will be contained in ECAL plus HCAL. We need…

Instrumentation and Detectors · Physics 2019-08-13 Shaojun Lu

In 1998, the detector H1 at HERA has been equipped with a small backward spectrometer, the Very Low Q^2 (VLQ) spectrometer comprising a silicon tracker, a tungsten - scintillator sandwich calorimeter, and a Time-of-Flight system. The…

Instrumentation and Detectors · Physics 2008-11-26 A. Stellberger , K. Meier , O. Niedermaier , O. Nix , K. Schmitt , J. Stiewe , M. Weber , J. Ferencei , F. Krivan , J. Spalek

When testing and calibrating particle detectors in a test beam, accurate tracking information independent of the detector being tested is extremely useful during the offline analysis of the data. A general-purpose Silicon Beam Tracker (SBT)…

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…

A simulation study of energy resolution, position resolution, and $\pi^0$-$\gamma$ separation using multivariate methods of a sampling calorimeter is presented. As a realistic example, the geometry of the calorimeter is taken from the…

Instrumentation and Detectors · Physics 2017-08-02 Ashim Roy , Shilpi Jain , Sunanda Banerjee , Satyaki Bhattacharya , Gobinda Majumder

The electromagnetic calorimeters of the various magnetic spectrometers in Hall C at Jefferson Lab are presented. For the existing HMS and SOS spectrometers design considerations, relevant construction information, and comparisons of…

We examine three dense high-Z scintillating crystals for the $\mu \to e$ conversion experiment using the GEANT4 simulation toolkit. The full energy deposition, albedo, and longitudinal and lateral energy leakages for all crystal assemblies…

Instrumentation and Detectors · Physics 2012-12-19 Zafar Usubov

Chromatic calorimetry (CCAL) analyses particle detection by utilizing scintillators with distinct emission wavelengths to measure the longitudinal energy deposition of particle showers in high-energy physics, improving particle…

High Energy Physics - Experiment · Physics 2025-09-12 Devanshi Arora

A small prototype of a finely granulated digital hadron calorimeter with Resistive Plate Chambers as active elements was exposed to positive pions of 1 >. 16 GeV energy from the Fermilab test beam. The event selection separates events with…

Instrumentation and Detectors · Physics 2015-05-14 Burak Bilki , John Butler , Georgios Mavromanolakis , Ed May , Edwin Norbeck , Jose Repond , David Underwood , Lei Xia , Qingmin Zhang

The electromagnetic calorimeter (ECAL) is a key detector component for precise electron and photon measurements in electron-ion collision experiments. At the Electron-Ion Collider in China (EicC), high-performance calorimetry is essential…

Instrumentation and Detectors · Physics 2026-03-23 Ye Tian , Souvik Maity , Jingyu Li , Yuancai Wu , Shan Sha , Yutie Liang , Aiqiang Guo , Yuxiang Zhao , Dexu Lin

Particle Flow Algorithms (PFAs) have been proposed as a method of improving the jet energy resolution of future colliding beam detectors. PFAs require calorimeters with high granularity to enable three-dimensional imaging of events. The…

Instrumentation and Detectors · Physics 2019-08-13 Kurt Francis

We investigate the three dimensional substructure of hadronic showers in the CALICE scintillator-steel hadronic calorimeter. The high granularity of the detector is used to find track segments of minimum ionising particles within hadronic…

Instrumentation and Detectors · Physics 2013-07-30 CALICE Collaboration , C. Adloff , J. -J. Blaising , M. Chefdeville , C. Drancourt , R. Gaglione , N. Geffroy , Y. Karyotakis , I. Koletsou , 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 , 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 , D. Dannheim , A. Dotti , G. Folger , V. Ivantchenko , W. Klempt , E. van der Kraaij , A. -I. Lucaci-Timoce , A. Ribon , D. Schlatter , V. Uzhinskiy , C. Carloganu , P. Gay , S. Manen , L. Royer , M. Tytgat , N. Zaganidis , 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 , O. Hartbrich , B. Hermberg , S. Karstensen , F. Krivan , K. Krüger , S. Lu , S. Morozov , V. Morgunov , M. Reinecke , F. Sefkow , P. Smirnov , M. Terwort , N. Feege , E. Garutti , S. Laurien , I. Marchesini , M. Matysek , M. Ramilli , K. Briggl , P. Eckert , T. Harion , H. -Ch. Schultz-Coulon , W. Shen , R. Stamen , B. Bilki , E. Norbeck , Y. Onel , G. W. Wilson , K. Kawagoe , Y. Sudo , T. Yoshioka , P. D. Dauncey , A. -M. Magnan , V. Bartsch , M. Wing , F. Salvatore , E. Cortina Gil , S. Mannai , G. Baulieu , P. Calabria , L. Caponetto , C. Combaret , R. Della Negra , G. Grenier , R. Han , J-C. Ianigro , R. Kieffer , I. Laktineh , N. Lumb , H. Mathez , L. Mirabito , A. Petrukhin , A. Steen , W. Tromeur , M. Vander Donckt , Y. Zoccarato , E. Calvo Alamillo , M. -C. Fouz , J. Puerta-Pelayo , F. Corriveau , 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. Rouene , N. Seguin-Moreau , M. Anduze , V. Balagura , V. Boudry , J-C. Brient , R. Cornat , M. Frotin , F. Gastaldi , E. Guliyev , Y. Haddad , F. Magniette , G. Musat , M. Ruan , T. H. Tran , 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 , K. Kotera , T. Takeshita , S. Uozumi , D. Jeans , M. Götze , J. Sauer , S. Weber , C. Zeitnitz