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Related papers: Charge sharing in single and double GEMs

200 papers

The research is aimed to address issues of analysis and mitigation of high repetition rate effects in Dielectric Wakefield Accelerators, and more specifically, to study charging rate and charge distribution in a thin walled dielectric…

Accelerator Physics · Physics 2015-10-20 S. V. Shchelkunov , T. C. Marshall , J. L. Hirshfield

We measured the properties of a novel combination of two Gas Electron Multipliers with a Micromegas for use as amplification devices in high-rate gaseous time projection chambers. The goal of this design is to minimize the buildup of space…

Instrumentation and Detectors · Physics 2016-09-21 S. Aiola , R. J. Ehlers , S. Gu , J. W. Harris , R. Majka , J. D. Mulligan , M. Oliver , J. Schambach , N. Smirnov

The ALICE experiment at LHC has planned to upgrade the TPC by replacing the MWPC with GEM based detecting elements to restrict the IBF to a tolerable value. However the variation of the gain as a function of physical parameters of…

Instrumentation and Detectors · Physics 2019-08-21 Supriya Das

The determination of the neutrino mass is an open issue in modern particle physics and astrophysics. The direct mass measurement is the only theory-unrelated experimental tool capable to probe such quantity. The HOLMES experiment aims to…

Background: we develop the concept of a Micromegas (MICRO-MEsh GAseous Structure) readout plane with an additional GEM (Gas Electron Multiplier) preamplification stage placed a few mm above it, to increase the maximum effective gain of the…

Sensitivities of current directional dark matter search detectors using gas time projection chambers are now constrained by target mass. A ton-scale gas TPC detector will require large charge readout areas. We present a first demonstration…

Instrumentation and Detectors · Physics 2020-11-24 A. C. Ezeribe , C. Eldridge , W. Lynch , R. R. Marcelo Gregorio , A. Scarff , N. J. C. Spooner

Gas Electron Multiplier (GEM)-based detectors using a layer of 10B as a neutron converter is becoming popular for thermal neutron detection. A common strategy to simulate this kind of detector is based on two frameworks: Geant4 and…

Instrumentation and Detectors · Physics 2022-12-21 R. Felix dos Santos , M. G. Munhoz , M. Moralles , L. A. Serra Filho , M. Bregant , F. A. Souza

Dual-phase liquid-xenon time projection chambers (LXe TPCs) deploying a few tonnes of liquid are presently leading the search for WIMP dark matter. Scaling these detectors to 10-fold larger fiducial masses, while improving their sensitivity…

Instrumentation and Detectors · Physics 2024-09-17 G. Martínez-Lema , A. Roy , A. Breskin , L. Arazi

The Gas Electron Multiplier (GEM) detectors has been utilized for various applications due to their excellent spatial resolution, high rate capabilities and flexibility in design. The GEM detectors stand as a promising device to be used in…

Instrumentation and Detectors · Physics 2020-02-21 Mohit Gola , Aashaq Shah , Asar Ahmed , Shivali Malhotra , Ashok Kumar , Md. Naimuddin

We review latest progress in gaseous photomultipliers (GPM) combining solid photocathodes and various types of novel electron multipliers. Cascaded gaseous electron multipliers (GEM) coated with CsI photocathodes can efficiently replace…

Instrumentation and Detectors · Physics 2009-11-13 R. Chechik , A. Breskin

Study of the uniformity of gain, energy resolution and count rate over active area of a triple GEM detector has been performed using a strong Fe55 X-ray source with premixed gas of Argon and CO2 in 70/30 ratio and conventional NIM…

Instrumentation and Detectors · Physics 2019-07-24 S. Chatterjee , S. Chakraborty , S. Roy , S. Biswas , S. Das , S. K. Ghosh , S. K. Prasad , S. Raha

Gas Electron Multiplier (GEM) technology is being considered for the forward muon upgrade of the CMS experiment in Phase 2 of the CERN LHC. Its first implementation is planned for the GE1/1 system in the $1.5 < \mid\eta\mid < 2.2$ region of…

Instrumentation and Detectors · Physics 2014-12-10 D. Abbaneo , M. Abbas , M. Abbrescia , A. A. Abdelalim , M. Abi Akl , W. Ahmed , W. Ahmed , P. Altieri , R. Aly , C. Asawatangtrakuldee , A. Ashfaq , P. Aspell , Y. Assran , I. Awan , S. Bally , Y. Ban , S. Banerjee , P. Barria , L. Benussi , V. Bhopatkar , S. Bianco , J. Bos , O. Bouhali , S. Braibant , S. Buontempo , C. Calabria , M. Caponero , C. Caputo , F. Cassese , A. Castaneda , S. Cauwenbergh , F. R. Cavallo , A. Celik , M. Choi , K. Choi , S. Choi , J. Christiansen , A. Cimmino , S. Colafranceschi , A. Colaleo , A. Conde Garcia , M. M. Dabrowski , G. De Lentdecker , R. De Oliveira , G. de Robertis , S. Dildick , B. Dorney , W. Elmetenawee , G. Fabrice , M. Ferrini , S. Ferry , P. Giacomelli , J. Gilmore , L. Guiducci , A. Gutierrez , R. M. Hadjiiska , A. Hassan , J. Hauser , K. Hoepfner , M. Hohlmann , H. Hoorani , Y. G. Jeng , T. Kamon , P. E. Karchin , H. S. Kim , S. Krutelyov , A. Kumar , J. Lee , T. Lenzi , L. Litov , F. Loddo , T. Maerschalk , G. Magazzu , M. Maggi , Y. Maghrbi , A. Magnani , N. Majumdar , P. K. Mal , K. Mandal , A. Marchioro , A. Marinov , J. A. Merlin , A. K. Mohanty , A. Mohapatra , S. Muhammad , S. Mukhopadhyay , M. Naimuddin , S. Nuzzo , E. Oliveri , L. M. Pant , P. Paolucci , I. Park , G. Passeggio , B. Pavlov , B. Philipps , M. Phipps , D. Piccolo , H. Postema , G. Pugliese , A. Puig Baranac , A. Radi , R. Radogna , G. Raffone , S. Ramkrishna , A. Ranieri , C. Riccardi , A. Rodrigues , L. Ropelewski , S. RoyChowdhury , M. S. Ryu , G. Ryu , A. Safonov , A. Sakharov , S. Salva , G. Saviano , A. Sharma , S. K. Swain , J. P. Talvitie , C. Tamma , A. Tatarinov , N. Turini , T. Tuuva , J. Twigger , M. Tytgat , I. Vai , M. van Stenis , R. Venditi , E. Verhagen , P. Verwilligen , P. Vitulo , D. Wang , M. Wang , U. Yang , Y. Yang , R. Yonamine , N. Zaganidis , F. Zenoni , A. Zhang

For its physics program with a high-intensity hadron beam of up to 2e7 particles/s, the COMPASS experiment at CERN requires tracking of charged particles scattered by very small angles with respect to the incident beam direction. While good…

A wire GEM (WGEM) detector with a gas gap between meshes was constructed. The detector provides the amplification 5x10E5 for the gas mixture of Ar +20% CO2 at atmospheric pressure. As compared with well-known GEM detectors produced by…

Instrumentation and Detectors · Physics 2009-11-26 B. M. Ovchinnikov , V. I. Razin , A. I. Reshetin , S. N. Filippov

We further study the performance of single, double and triple Gas Electron Multiplier (GEM) detectors in pure noble gases at high pressures, in the range of 1-10 atm. We confirm that light noble gases, in particular He and its mixtures with…

Instrumentation and Detectors · Physics 2015-06-26 V. Aulchenko , A. Bondar , A. Buzulutskov , L. Shekhtman , R. Snopkov , Yu. Tikhonov

Many experiments are currently using or proposing to use large area GEM foils in their detectors, which is creating a need for commercially available GEM foils. Currently CERN is the only main distributor of large GEM foils, however with…

Instrumentation and Detectors · Physics 2018-06-07 M. Posik , B. Surrow

A novel and relatively simple method of production of electrodes for a multi-channel wire gas multiplier is developed. Two modifications of the multipliers have been tested: with a multiplication of electrons between two wire electrodes,…

Instrumentation and Detectors · Physics 2010-11-15 B. M. Ovchinnikov , V. V. Parusov , Yu. B. Ovchinnikov

Optical readout of large Time Projection Chambers (TPCs) with multiple Gas Electron Multipliers (GEMs) amplification stages has shown to provide very interesting performances for high energy particle tracking. Proposed applications for…