Measurements of Stability of Gas Electron Multiplier (GEM)

Slides:



Advertisements
Similar presentations
GEM Chambers at BNL The detector from CERN, can be configured with up to 4 GEMs The detector for pad readout and drift studies, 2 GEM maximum.
Advertisements

Cosmic Ray Test of GEM- MPI/TPC in Magnetic Field Hiroshima University Kuroiwa CDC Group Mar
Status of test beam data analysis … with emphasis on resistive coating studies Progress and questions 1Meeting at CEA Saclay, 25 Jan 2010Jörg Wotschack,
Present Status of GEM Detector Development for Position Counter 1.Introduction 2.GEM 3.Readout Board 4.Fabrication Test 5.Large GEM 6.Readout Electronics.
1 MUON TRACKER FOR CBM experiment Murthy S. Ganti, VEC Centre Detector Choice.
GEM Detector Shoji Uno KEK. 2 Wire Chamber Detector for charged tracks Popular detector in the particle physics, like a Belle-CDC Simple structure using.
Update on GEM-based DHCAL for SiD Andy White For GEM/DHCAL Group September 21, 2005.
1 Alhussein Abuhoza, S. Biswas, U. Frankenfeld, J. Hehner, Ch. Schmidt GSI, Darmstadt, Germany and H.R. Schmidt University of Tübingen, Germany Study of.
IHEP, Bejing 9th ACFA ILC Physics and Detector Workshop & ILC GDE Meeting The preliminary results of MPGD-based TPC performance at KEK beam.
1 The GEM Readout Alternative for XENON Uwe Oberlack Rice University PMT Readout conversion to UV light and proportional multiplication conversion to charge.
Development of a Time Projection Chamber Using Gas Electron Multipliers (GEM-TPC) Susumu Oda, H. Hamagaki, K. Ozawa, M. Inuzuka, T. Sakaguchi, T. Isobe,
GEM: A new concept for electron amplification in gas detectors Contents 1.Introduction 2.Two-step amplification: MWPC combined with GEM 3.Measurement of.
Yosuke Watanabe….. University of Tokyo, RIKEN A, KEK C, Development of a GEM tracker for E16 J-PARC 1 Thanks to ???????????
Semester Project: Linear Collider Beam Test Data Analysis PHYS 5326 Spring 2007 Jacob Smith.
TPC R&D status in Japan T. Isobe, H. Hamagaki, K. Ozawa, and M. Inuzuka Center for Nuclear Study, University of Tokyo Contents 1.Development of a prototype.
EPS-HEP 2015, Vienna. 1 Test of MPGD modules with a large prototype Time Projection Chamber Deb Sankar Bhattacharya On behalf of.
5 th RD51 meeting (WG1) 25 May 2009 Atsuhiko Ochi ( Kobe University )
Experimental and Numerical studies on Bulk Micromegas SINP group in RD51 Applied Nuclear Physics Division Saha Institute of Nuclear Physics Kolkata, West.
12/12/09 MPGD 神戸大学 1 Yusuke Komatsu A B. Azmoun B, C. Woody B, K. Ozawa A University of Tokyo A,Brook Haven National Lab. B.
GEM basic test and R&D plan Takuya Yamamoto ( Saga Univ. )
1/18 01/26/2007MPGD Workshop in Saga (Yorito Yamaguchi, CNS, Univ. of Tokyo) 東大 CNS における GEM の基本動 作特性の研究 Measurement of basic properties of GEM at CNS,
Atsushi Aoza ( saga University ) A Simulation Study of GEM gating at ILC-TPC A.Ishikawa, A.Sugiyama, H.Fujishima, K.Kadomatsu(Saga U.) K.Fujii,M.Kobayashi,
Taku Gunji Center for Nuclear Study The University of Tokyo
Design and performance of Active Target GEM-TPC R. Akimoto, S. Ota, S, Michimasa, T. Gunji, H. Yamaguchi, T. hashimoto, H. Tokieda, T. Tsuji, K. Kawase,
1 GEM R&D Activity in USTC Yi Zhou University of Science & Technology of China.
Future Possibilities for Measuring Low Mass Lepton Pairs in Christine Aidala for the Collaboration Quark Matter 2002, Nantes.
Triple GEM Beam Test within PHENIX DC Upgrades Meeting 4/14/04 B. Azmoun PHENIX Brookhaven National Lab.
30 October 2003V.Souvorov / B.Schmidt - MWPC PRR CERN site1 MWPC Aging Studies Outline: Overview of aging tests done Results in terms of gain variations.
UTA Digital hadron Calorimetry using the GEM concept J.Li, A.White, J.Yu 5/30/02.
1 HBD R&D: Update Itzhak Tserruya (for A. Kozlov, I. Ravinovich and L. Shekhtman) Weizmann Institute, Rehovot DC meeting Feb. 14, 2003.
J-PARC での高輝度 ビームに向けた GEM トラッカーの 開発 小沢 恭一郎 ( 東大・理 ) KEK 測定器開発室 Supported by 科研費.
Section 2: Electric Field Properties. What is an electric field: Gravitational Fields Affect anything that has:_____ Strong Gravitational fields come.
Results on a Large Area triple-GEM Detector at LNF 5 th RD51 Collaboration Meeting Freiburg, 25 May 2010 D. Domenici - LNF.
Gas Electron Multiplier
GEM-MSTPC for direct measurements of astrophysical reaction rates H. Ishiyama 1, K. Yamaguchi 2, Y. Mizoi 3, Y.X. Watanabe 1, T. Hashimoto 4, M.H. Tanaka.
Status of the ALICE TPC upgrade C. Garabatos. Running at 50 kHz Pb-Pb after LS2 No GG triggering, continuous readout This leads to electric field distortions.
Thorsten Lux. Charged particles X-ray (UV) Photons Cathode Anode Amplification Provides: xy position Energy (z position) e- CsI coating 2 Gas (Mixture)
R&D on Hadron Blind detector, recent results Issues addressed: - gain limits in CF 4 with heavily ionizing particles - operation.
Development of an active target for astrophysical experiments at CRIB Takashi Hashimoto The University of Tokyo, CNS.
Design and performance of Active Target GEM-TPC R. Akimoto, S. Ota, S, Michimasa, T. Gunji, H. Yamaguchi, T. Hashimoto, H. Tokieda, T. Tsuji, S. Kawase,
R&D activities on a double phase pure Argon THGEM-TPC A. Badertscher, A. Curioni, L. Knecht, D. Lussi, A. Marchionni, G. Natterer, P. Otiougova, F. Resnati,
Hardware considerations about Ar vs. Ne
GEM and MicroMegas R&D Xiaomei Li Science and Technology
Activity of CERN and LNF Groups on Large Area GEM Detectors
some thoughts on charging-up effects
A slow control system for a
Single GEM Measurement
Updates on the Micromegas + GEM prototype
Micropattern Gas Detectors
Digital Calorimetry using GEM technology Andy White for UTA group
Development of Hard X-ray Detector with GEM
Numerical simulations on single mask conical GEMs
Potential Ion Gate using GEM: experiment and simulation
Numerical simulations on single mask conical GEMs
Development of Gas Electron Multiplier Detectors for Muon Tomography
Dan Burke1, P. Colas2, M. Dixit1, I. Giomataris2, V. Lepeltier3, A
MWPC’s, GEM’s or Micromegas for AD transfer and experimental lines
Development of GEM at CNS
Development of gating foils using FPC production techniques
The study of GEM detector based on APV25 at CIAE
Numerical simulations on single mask conical GEMs
Calculate work done by expanding gas of 1 mole if initial pressure is 4000 Pa, initial volume is 0.2 m3. Assume a two processes: (1) isobaric expansion.
(On Behalf of CMS Muon Group)
The first signal of GEM-TPC
Production of a 3D-Printed THGEM Board
Construction and Test of a Modular GEM for EIC
The MPPC Study for the GLD Calorimeter Readout
Gain measurements of Chromium GEM foils
A DLC μRWELL with 2-D Readout
Gaseous detectors at the LHC experiments: GEM technology (lesson #3)
Presentation transcript:

Measurements of Stability of Gas Electron Multiplier (GEM) Y.L. Yamaguchi, H. Hamagaki, K. Ozawa, S.X. Oda, M. Inuzukaa, S.Sanob CNS,Univ. of Tokyo, National Research Institute for Cultural Properties Tokyoa, Waseda Univ.b 9/21/2005 DNP/JPS meeting in Hawaii

DNP/JPS meeting in Hawaii Contents Introduction Gas Electron Multiplier (GEM) Characteristics of CNS-GEM and CERN-GEM Aim of the study Experimental setup for measurements Results P/T dependence of gain Gain stability CNS-GEM and CERN-GEM Ar-CH4 and Ar-CO2 Summary 9/21/2005 DNP/JPS meeting in Hawaii

DNP/JPS meeting in Hawaii Gas Electron Multiplier (GEM) GEM is originally invented by F.Sauli @CERN. Structure A metalized polymer foil with holes (Cu:5mm + Kapton:50mm + Cu:5mm ) Hole : pitch @ 100mm f @ 50mm A photograph of GEM Insulator Mechanism of signal amplification A micrograph of GEM VGEM is applied between the metal layers. When an electron passes through the hole on GEM, strong electric field inside the hole induces the cascade of electrons. VGEM 50mm 100mm GEM can be an upgrade for a wire chamber. Electric field inside holes 9/21/2005 DNP/JPS meeting in Hawaii

DNP/JPS meeting in Hawaii Characteristics of CNS-GEM and CERN-GEM We succeeded in fabricating a new type of GEM (CNS-GEM) using a dry etching method. CERN-GEM CNS-GEM Etching method wet etching dry etching The cross section of a hole A hole with double-conical shape A hole with cylindrical shape 9/21/2005 DNP/JPS meeting in Hawaii

DNP/JPS meeting in Hawaii Aim of the study Measure basic properties of CNS-GEM. Gain P/T dependence Stability Known problem on gain stability It has been reported that gas gain of CERN-GEM increases (or decreases) as a function of illumination time. A. Orthen et al.,NIM A 512 (2003) 476 Possible reason Due to shape of holes of GEM Charge up of the Kapton surface inside the holes. CERN-GEM CNS-GEM CNS-GEM is expected to have better stability than CERN-GEM. 9/21/2005 DNP/JPS meeting in Hawaii

DNP/JPS meeting in Hawaii Experimental setup for the measurements 55Fe(X-ray,5.9 keV) HV1 Mesh P/T dependence of gain Gain stability CNS-GEM,CERN-GEM Ar-CH4 (Ar : CH4 = 90 : 10) Ar-CO2 (Ar : CO2 = 70 : 30) HV2 3mm 1MΩ 10MW GEM 3 10MW 1MΩ 2mm 1MΩ 10MW GEM 2 1MΩ 10MW 1MΩ 2mm GEM 1 10MW 2mm 10MW 1MΩ PAD VME ADC PreAmp 9/21/2005 DNP/JPS meeting in Hawaii

DNP/JPS meeting in Hawaii P/T dependence of gain (CERN-GEM) Gain is measured as a function of P/T. Pressure is manually changed during the measurement. Correlation function is evaluated as the formula below. CERN-GEM Ar-CH4 Assumed correlation function is good agreement with the measurements. 9/21/2005 DNP/JPS meeting in Hawaii

DNP/JPS meeting in Hawaii P/T dependence of gain (CNS-GEM) 0.1% fluctuation of P/T causes about 1% fluctuation of gain. The effect of P/T on gain is less than 1%. P/T is stable within 0.1% during our measurements. Ar-CH4 Ar-CO2 CNS-GEM CNS-GEM 9/21/2005 DNP/JPS meeting in Hawaii

Gain stability of CERN-GEM Gain stability of CERN-GEM is measured as a baseline. Increasing of gain as a function of illumination time is clearly seen. A difference of gain stability between Ar-CO2 and Ar-CH4 is observed. Further study is underway. 9/21/2005 DNP/JPS meeting in Hawaii

DNP/JPS meeting in Hawaii Gain stability of CNS-GEM (Ar-CH4) CNS-GEM shows very good stability!! CNS-GEM is stable within error of the measurement. 9/21/2005 DNP/JPS meeting in Hawaii

DNP/JPS meeting in Hawaii Gain stability of CNS-GEM (Ar-CO2) The case of Ar-CO2 is similar to that of Ar-CH4. The gain stability of CNS-GEM is better than that of CERN-GEM. The shape of holes in GEM significantly affect gain stability. 9/21/2005 DNP/JPS meeting in Hawaii

DNP/JPS meeting in Hawaii Summary P/T dependence and stability of gain have been measured. Assumed correlation function between gain and P/T is good agreement with the measurements. A difference of gain stability between Ar-CO2 and Ar-CH4 is observed. Further study is underway. The gain stability of CNS-GEM is better than that of CERN-GEM. The shape of holes in GEM significantly affect gain stability. 9/21/2005 DNP/JPS meeting in Hawaii