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Optical readout of GEM based devices by means of high granularity and low noise CMOS sensors allows to obtain very interesting tracking performance. Space resolution of the order of tens of $\mu$m were measured on the GEM plane along with…

A prototype Dual Gain Multilayer Thick Gas Electron Multilyer (DG-M-THGEM) with an active area of 10 cm $\times$ 10 cm was manufactured aiming at the production of a large-volume active-target time projection chamber which can work under…

Gas detector are very light instrument used in high energy physics to measure the particle properties: position and momentum. Through high electric field is possible to use the Gas Electron Multiplier (GEM) technology to detect the…

The construction of a micro-pattern gas detector of dimensions 40x10 cm**2 is described. Two gas electron multiplier foils (GEM) provide the internal amplification stages. A two-layer readout structure was used, manufactured in the same…

In CBM Experiment at FAIR, dimuons will be detected by a Muon Chamber (MUCH) consisting of segmented absorbers of varying widths and tracking chambers sandwiched between the absorber-pairs. In this fixed target heavy-ion collision…

Instrumentation and Detectors · Physics 2016-06-03 Rama Prasad Adak , Ajit Kumar , A. K. Dubey , Subhasis Samanta , J. Saini , S. Das , S. Raha , Subhasis Chattopadhyay

We study the performance of gaseous and two-phase (liquid-gas) cryogenic detectors of ionizing radiation, based on gas electron multipliers (GEMs). For the first time, high gas gains, exceeding 10^4, were obtained in pure He, Ar and Kr at…

Instrumentation and Detectors · Physics 2009-11-10 A. Buzulutskov , A. Bondar , L. Shekhtman , R. Snopkov , Y. Tikhonov

A MicroCAT (Micro Compteur A Trous) structure which is used for avalanche charge multiplication in gas filled radiation detectors has been optimised with respect to maximum electron transparency and minimum ion feedback. We report on the…

Instrumentation and Detectors · Physics 2009-11-10 A. Orthen , H. Wagner , H. J. Besch , R. H. Menk , A. H. Walenta , U. Werthenbach

After the Phase-2 high-luminosity upgrade to the Large Hadron Collider (LHC), the collision rate and therefore the background rate will significantly increase, particularly in the high $\eta$ region. To improve both the tracking and…

Instrumentation and Detectors · Physics 2021-12-08 M. Abbas , M. Abbrescia , H. Abdalla , A. Abdelalim , S. AbuZeid , A. Agapitos , A. Ahmad , A. Ahmed , W. Ahmed , C. Aimè , C. Aruta , I. Asghar , P. Aspell , C. Avila , J. Babbar , Y. Ban , R. Band , S. Bansal , L. Benussi , V. Bhatnagar , M. Bianco , S. Bianco , K. Black , L. Borgonovi , O. Bouhali , A. Braghieri , S. Braibant , S. Butalla , S. Calzaferri , M. Caponero , J. Carlson , F. Cassese , N. Cavallo , S. S. Chauhan , S. Colafranceschi , A. Colaleo , A. Conde Garcia , M. Dalchenko , A. De Iorio , G. De Lentdecker , D. Dell Olio , G. De Robertis , W. Dharmaratna , S. Dildick , B. Dorney , R. Erbacher , F. Fabozzi , F. Fallavollita , A. Ferraro , D. Fiorina , E. Fontanesi , M. Franco , C. Galloni , P. Giacomelli , S. Gigli , J. Gilmore , M. Gola , M. Gruchala , A. Gutierrez , R. Hadjiiska , T. Hakkarainen , J. Hauser , K. Hoepfner , M. Hohlmann , H. Hoorani , T. Huang , P. Iaydjiev , A. Irshad , A. Iorio , F. Ivone , W. Jang , J. Jaramillo , A. Juodagalvis , E. Juska , B. Kailasapathy , T. Kamon , Y. Kang , P. Karchin , A. Kaur , H. Kaur , H. Keller , H. Kim , J. Kim , S. Kim , B. Ko , A. Kumar , S. Kumar , N. Lacalamita , J. S. H. Lee , A. Levin , Q. Li , F. Licciulli , L. Lista , K. Liyanage , F. Loddo , M. Luhach , M. Maggi , Y. Maghrbi , N. Majumdar , K. Malagalage , S. Malhotra , S. Martiradonna , C. McLean , J. Merlin , M. Misheva , G. Mocellin , L. Moureaux , A. Muhammad , S. Muhammad , S. Mukhopadhyay , M. Naimuddin , S. Nuzzo , R. Oliveira , P. Paolucci , I. C. Park , L. Passamonti , G. Passeggio , A. Peck , A. Pellecchia , N. Perera , L. Petre , H. Petrow , D. Piccolo , D. Pierluigi , G. Raffone , M. Rahmani , F. Ramirez , A. Ranieri , G. Rashevski , B. Regnery , M. Ressegotti , C. Riccardi , M. Rodozov , E. Romano , C. Roskas , B. Rossi , P. Rout , J. D. Ruiz , A. Russo , A. Safonov , A. K. Sahota , D. Saltzberg , G. Saviano , A. Shah , A. Sharma , R. Sharma , T. Sheokand , M. Shopova , F. M. Simone , J. Singh , U. Sonnadara , E. Starling , B. Stone , J. Sturdy , G. Sultanov , Z. Szillasi , D. Teague , D. Teyssier , T. Tuuva , M. Tytgat , I. Vai , N. Vanegas , R. Venditti , P. Verwilligen , W. Vetens , A. K. Virdi , P. Vitulo , A. Wajid , D. Wang , K. Wang , I. J. Watson , N. Wickramage , D. D. C. Wickramarathna , S. Yang , U. Yang , Y. Yang , J. Yongho , I. Yoon , Z. You , I. Yu , S. Zaleski

Advances in fabrication techniques and high-performance electronics have facilitated the development of fine-pitch Gas Electron Multipliers (GEMs). Earlier experimental and simulation findings suggest that these reduced-pitch GEMs can…

Instrumentation and Detectors · Physics 2026-01-16 Rajiv Gupta , Sunidhi Saxena , Ajay Kumar

A simple methodology for evaluating the dynamic-range of gas avalanche detectors in the laboratory is presented and discussed. It comprises two tools: a charge injector of tunable gain which transfers radiation-induced amplified electron…

Instrumentation and Detectors · Physics 2015-06-17 S. Bressler , L. Moleri , L. Arazi , E. Erdal , A. Rubin , M. Pitt , A. Breskin

We present a gas selection for Xe-based gas electron multiplier (GEM) detectors, Gas Multiplier Counters (GMCs) onboard the CubeSat X-ray observatory NinjaSat. To achieve an energy bandpass of 2-50 keV, we decided to use a Xe-based gas…

A large-area and light-weight Gas Electron Multiplier (GEM) detector was built at the University of Virginia as a prototype for the detector R$\&$D program of the future Electron Ion Collider. The prototype has a trapezoidal geometry…

Instrumentation and Detectors · Physics 2025-07-03 Kondo Gnanvo , Xinzhan Bai , Chao Gua , Nilanga Liyanage , Vladimir Nelyubin , Yuxiang Zhao

With the intention of creating a complete simulation of the Thick GEM detector, this work presents a partial simulation of the interaction of 6 keV X-Ray radiation with a gas volume. For the gas, it was used pure Argon, Xenon and CO2 as…

Instrumentation and Detectors · Physics 2021-10-05 Lucas Maia Rios , Mauro R. Cosentino

Gas electron multipliers (GEMs) have been overcoated with a high resistivity 10e14 - 10e15 Ohms / square amorphous carbon layer. The coating avoids charging up of the holes and provides a constant gain immediately after switching on…

Instrumentation and Detectors · Physics 2008-11-26 S. Beirle , U. Werthenbach , G. Zech , T. Zeuner

A large number of high-energy and heavy-ion experiments successfully used Time Projection Chamber (TPC) as central tracker and particle identification detector. However, the performance requirements on TPC for new high-rate particle…

Instrumentation and Detectors · Physics 2013-02-14 M. Poli Lener , M. Bazzi , G. Corradi , C. Curceanu , A. D'Uffizi , C. Paglia , A. Romero Vidal , E. Sbardella , A. Scordo , D. Tagnani , J. Zmeskal

The Gas Electron Multiplier (GEM) is a new age detector, which can handle the high flux of particles. The GEM foil, which is constructed using 50$\mu$m highly insulating foil (Kapton/Apical) coated with 5$\mu$m layers of copper, on both…

Instrumentation and Detectors · Physics 2022-05-10 Asar Ahmed , Ashok Kumar , Md. Naimuddin , Michal Babij , Piotr Bielowka

Optical readout of Gas Electron Multipliers (GEM) provides very interesting performances and has been proposed for different applications in particle physics. In particular, thanks to its good efficiency in the keV energy range, it is being…

An approximate formula has been derived for gain fluctuations in cascaded gaseous detectors such as GEM-s, based on the assumption that the charge collection, avalanche formation and extraction steps are independent cascaded processes. In…

Instrumentation and Detectors · Physics 2016-08-24 Dezső Varga

We have developed a new design of a GEM-like detector with single-layer electrodes made of a resistive kapton. This detector can operate at gains close to 10E5 even in pure Ar and Ne and if transited to discharges at higher gains they, due…

Plasma Physics · Physics 2008-11-26 R. Oliveira , V. Peskov , F. Pietropaolo , P. Picchi
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