TCPD test measurement 1 TCPD (TGEM CCC Photon Detector) test measurement ELTE, MTA KFKI RMKI, REGARD Group (Budapest, Hungary): Levente Kovács G. Hamar,

Slides:



Advertisements
Similar presentations
General Characteristics of Gas Detectors
Advertisements

Radiation Detection ionization chambers (dosimeters, pulse chambers, particle track chambers) scintillation detectors semiconductor detectors photographic.
Geiger Counters. Higher Voltage As the voltage increases in a gas detector the ions collected increases. The proportional region ends. –Streamer mode.
Geiger-Muller detector and Ionization chamber
Drift velocity Adding polyatomic molecules (e.g. CH4 or CO2) to noble gases reduces electron instantaneous velocity; this cools electrons to a region where.
Aging, High Rate and Shielding L. Lopes Lip-Coimbra.
1 Sep. 19, 2006Changguo Lu, Princeton University Induced signal in RPC, Configuration of the double gap RPC and Grouping of the strips Changguo Lu Princeton.
Prototype TPC Tests C. Lu 12/9/98 V = 0. Gas gain test for the low pressure chamber The chamber is constructed with the following parameters: D anode.
New Readout Methods for LAr detectors P. Otyugova ETH Zurich, Telichenphysik CHIPP Workshop on Neutrino physics.
Proportional Counters
Ionization. Measuring Ions A beam of charged particles will ionize gas. –Particle energy E –Chamber area A An applied field will cause ions and electrons.
Type of Material: Instrumentation Review
Chapter 6 Photodetectors.
Photon detection Visible or near-visible wavelengths
Kolympari, Crete, June 16, Study of avalanche fluctuations and energy resolution with an InGrid-TimePix detector P. Colas Progress report, based.
Measurement of gas gain fluctuations M. Chefdeville, LAPP, Annecy TPC Jamboree, Orsay, 12/05/2009.
C.Shalem et al, IEEE 2004, Rome, October 18 R. Chechik et al. ________________RICH2004_____________ Playa del Carmen, Mexico 1 Thick GEM-like multipliers:
Status of DRIFT II Ed Daw representing the DRIFT collaboration: Univ. of Sheffield, Univ. of Edinburgh, Occidental College, Univ. of New Mexico Overview.
Cube Measurements Tent Crew. Scintillation BNL 241 Am Semi- collimated  Spectralon Diffuse UV Reflector SBD  -Trigger Scint. Light Poisson.
SCINTILLATION COUNTER. PRINCIPLE When light radiations strike fluorescent material it produces flashes of light called scintillations. These are detected.
PHENIX Drift Chamber operation principles Modified by Victor Riabov Focus meeting 01/06/04 Original by Sergey Butsyk Focus meeting 01/14/03.
GEM: A new concept for electron amplification in gas detectors Contents 1.Introduction 2.Two-step amplification: MWPC combined with GEM 3.Measurement of.
Sheffield : R. Hollingworth, D. Tovey R.A.L. : R.Luscher Development of Micromegas charge readout for two phase Xenon based Dark Matter detectors Contents:
1 TRD-prototype test at KEK-FTBL 11/29/07~12/6 Univ. of Tsukuba Hiroki Yokoyama The TRD prototype is borrowed from GSI group (thanks Anton).
1 Development of Multi-Pixel Photon Counters (1) S.Gomi, T.Nakaya, M.Yokoyama, M.Taguchi, (Kyoto University) T.Nakadaira, K.Yoshimura, (KEK) Oct
Ionization Detectors Basic operation
Micromegas TPC Beam Test Result H.Kuroiwa (Hiroshima Univ.) Collaboration with Saclay, Orsay, Carlton, MPI, DESY, MSU, KEK, Tsukuba U, TUAT, Kogakuin U,
Experimental and Numerical studies on Bulk Micromegas SINP group in RD51 Applied Nuclear Physics Division Saha Institute of Nuclear Physics Kolkata, West.
Techniques for Nuclear and Particle Physics Experiments By W.R. Leo Chapter Eight:
MPPC status M.Taguchi(kyoto) T2K ND /7/7.
Summer Student Session, 11/08/2015 Sofia Ferreira Teixeira Summer Student at ATLAS-PH-ADE-MU COMSOL simulation of the Micromegas Detector.
2002 LHC days in Split Sandra Horvat 08 – 12 October, Ruđer Bošković Institute, Zagreb Max-Planck-Institute for Physics, Munich Potential is here...
Performance of new MPPC Nov. 21 Korea-Japan joint meeting Takashi Maeda Hideki Yamazaki Yuji Sudo (University of Tsukuba) --- Contents ---
Collection of Photoelectrons from a CsI Photocathode in Triple GEM Detectors C. Woody B.Azmuon 1, A Caccavano 1, Z.Citron 2, M.Durham 2, T.Hemmick 2, J.Kamin.
T. Zerguerras- RD51 WG Meeting- CERN - February Single-electron response and energy resolution of a Micromegas detector T. Zerguerras *, B.
S.S.GaO. Outline Introduction Experiment Results and discussion Conclusion References.
1 Analysis of Small RPC DHCAL Prototype Data (noise and cosmic ray) LCWA09, Albuquerque, New Mexico Friday, October 02, 2009 Qingmin Zhang HEP Division,
Group Meeting TPC 的基本原理 S.C.CHO.. TPC 的介紹 ionization electrons drift  wire chambers  avalanches position dependence of the induced signal  the point.
1 A two-phase Ar avalanche detector with CsI photocathode: first results A. Bondar, A. Buzulutskov, A. Grebenuk, D. Pavlyuchenko, R. Snopkov, Y. Tikhonov.
1 Fulvio TESSAROTTO GDD meeting, CERN, 01/10/2008 Trieste THGEM news New THGEM test in the COMPASS hall New THGEM test in the COMPASS hall Preparation.
Development of a Single Ion Detector for Radiation Track Structure Studies F. Vasi, M. Casiraghi, R. Schulte, V. Bashkirov.
RPCs with Ar-CO2 mix G. Aielli; R.Cardarelli; A. Zerbini For the ATLAS ROMA2 group.
R&D on Hadron Blind detector, recent results Issues addressed: - gain limits in CF 4 with heavily ionizing particles - operation.
Performance of 1600-pixel MPPC for the GLD Calorimeter Readout Jan. 30(Tue.) Korea-Japan Joint Shinshu Univ. Takashi Maeda ( Univ. of Tsukuba)
Part-II Wire type detectors 1. Single wire counters.
Space Charge Effects and Induced Signals in Resistive Plate Chambers
Development of Multi-Pixel Photon Counters (1)
Electronics & Communication Engineering
Fabio, Francesco, Francesco and Nicola INFN and University Bari
NUV-SiPM short technology description
Simulation of Properties of COMPASS Drift-Chamber Prototypes
Acknowledgements Slides and animations were made by Dr. Jon Karty Mass Spectrometry Facility Indiana University, Bloomington.
From: A fast high-voltage switching multiwire proportional chamber
THGEM: Introduction to discussion on UV-detector parameters for RICH
Photodetectors.
Gaseous Beam Position Detectors, with Low Cost and Low Material Budget
Radiation Detectors : Detection actually means measurement of the radiation with its energy content and other related properties. The detection system.
Upgrade of LXe gamma-ray detector in MEG experiment
Ionization detectors ∆
MWPC’s, GEM’s or Micromegas for AD transfer and experimental lines
R&D of MPPC for T2K experiment
Factors Limiting the Linearity of Response of Tissue Equivalent Proportional Counters Used in Micro- and Nano – Dosimetry T.Z. Kowalski i AGH, University.
Pre-installation Tests of the LHCb Muon Chambers
Geiger-Mueller Tubes By: Daniel Hancock.
Engineering Design Review
Micro Resistive Well Detector for Large Area Tracking
The MPPC Study for the GLD Calorimeter Readout
Gain measurements of Chromium GEM foils
Presentation transcript:

TCPD test measurement 1 TCPD (TGEM CCC Photon Detector) test measurement ELTE, MTA KFKI RMKI, REGARD Group (Budapest, Hungary): Levente Kovács G. Hamar, M. Mátyás D. Varga G. Hamar, M. Mátyás D. Varga Zimányi Winter School 2011, Budapest

2 TCPD test measurement Contents Chamber structure - motvationChamber structure - motvation Measurements with beta sourceMeasurements with beta source Ion and electron dirft in the chamberIon and electron dirft in the chamber Measurements with UV LEDMeasurements with UV LED Single photoelectron (PE) charge distributionSingle photoelectron (PE) charge distribution Photoelectrons & gain vs high voltagePhotoelectrons & gain vs high voltage (TGEM, SW) SummarySummary

3 Chamber structure - motivation Optimal matching of two amplifier stages (TGEM- and CCC- ). Optimal matching of two amplifier stages (TGEM- Thick Gas Electron Multiplier and CCC- Close Cathode Chamber). TGEM acts as electron pre-amplifier (gain ). TGEM acts as electron pre-amplifier (gain ). CCC (MWPC- ) works as further amplifier (gain ). CCC (MWPC- Multi Wire Proportional Chamber) works as further amplifier (gain ). Ion currents reflect field configuration. Ion currents reflect field configuration. Principle aim: to detect a single photoelectron with the TCPD chamber! Principle aim: to detect a single photoelectron with the TCPD chamber! TCPD test measurement

4 Main sections of the chamber (chamber structure) Three sections : Between cathode and TGEM: drift region. TGEM (preamplifier). Between bottom of the TGEM and the wire plane: extraction region. Readout TCPD test measurement

Electrostatic field in the TGEM- CCC & Chamber design 5 TCPD test measurement

6 Ion and electron drift in the chamber (whit beta & UV LED sorce) Avalanches are induced by single electrons (from ionization or PE) (UV LED). Continuous current is observable from ions drifting upwards (Beta). Typical voltage setting - charges Ions potentially cause ageing on the TGEM surface.

7 TCPD test measurement Ion currents as function of the extraction field Beta source used for irradiation. Low field: all currents go to the Field Wires (red line). Higher field: currents to go the TGEM top (green), focusing effect. Very high extraction field: currents go to the TGEM bottom (blue). Cathode: always low currents (purple).

Single photoelectron charge distribution (UV LED pulses) Avalanche statistics: single electron gives exponential total charge (very high fluctuation).Avalanche statistics: single electron gives exponential total charge (very high fluctuation). Exponential fit: area gives PE count, slope proportional to total amplification.Exponential fit: area gives PE count, slope proportional to total amplification. Often the Pólya distribution is used as approximation. Often the Pólya distribution is used as approximation. The total photoelectron per event is kept low (0.1 – 0.3 / event) to obtain the real single PE response. 8 TCPD test measurement

9 Single PE charge distribution vs. TGEM voltage Shape of the curves are conformal. Increasing TGEM voltage increases efficiency (not only signal / noise ratio). Departure from exponential becomes prominent at low charges. ( fix TGEM =1100 Volts) TCPD test measurement

10 Total amplification gain vs. TGEM and CCC voltages Upper panel: Gain vs. TGEM voltage. Lower panel: Gain vs. CCC sense wire voltage. Gain is exponential as a fuction of both variables, reflecting that the gain can be balanced between the two stages. No difference between UV LED and Beta source measurements: no saturation in the high gain (single electron sensitive) mode. TCPD test measurement

11 Photoelectron yield vs TGEM and CCC voltages Expectation: the PE number does not change with the sense wire voltages (but the gain does!) Photoelectron count development as a function of TGEM voltage (lower figure) The PE count after an initial exponential increase saturates at TGEM=1000 volts. Finding (measured data): There is some shallow dependence on TGEM voltage, due to improving PE extraction from TGEM surface. No dependence within error margines on CCC sense wire voltage. TCPD test measurement

12 Summary Single photoelectron detection possibility demonstrated with high signal / noise ratio. Single photoelectron detection possibility demonstrated with high signal / noise ratio. Two stage amplification (TGEM and CCC): increased stability and gain control. Two stage amplification (TGEM and CCC): increased stability and gain control. Ion back flow follows expected trends, gives information on internal electrical field. Ion back flow follows expected trends, gives information on internal electrical field. We have detected single photoelectrons with the first TCPD chamber. We have detected single photoelectrons with the first TCPD chamber. Applicability in different gas compositions (measurements with different gas mixtures see M.Matyas’ talk). Applicability in different gas compositions (measurements with different gas mixtures see M.Matyas’ talk). TCPD test measurement

Thank you for your attention! TCPD test measurement