CSC Test Beam Data Analysis Alexander Khodinov and Valeri Tcherniatine.

Slides:



Advertisements
Similar presentations
Triple-GEM detector operation for high-rate particle triggering W. Bonivento, G. Bencivenni, A. Cardini, C. Deplano, P. de Simone, F. Murtas, D. Pinci,
Advertisements

INFN Milano, Universita` degli Studi Milano Bicocca Siena IPRD May Testbeam results of the CMS electromagnetic calorimeter Alessio Ghezzi.
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.
Scintillator Tile Hadronic Calorimeter Prototype (analog or semidigital) M.Danilov ITEP(Moscow) CALICE Collaboration LCWS04, Paris.
Developments of micromegas detector at CERN/Saclay
Results from first tests of TRD prototypes for CBM DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Frankfurt am Main.
Behaviour of MicroMega chambers in magnetic field: analysis of H2 June data Outline: (0) Introduction (1) Data set used and noise filtering (2)Cluster.
Bulk Micromegas Our Micromegas detectors are fabricated using the Bulk technology The fabrication consists in the lamination of a steel woven mesh and.
Preshower 15/03/2005 P.Kokkas Preshower September Run Data Analysis P. Kokkas.
Track Fitting and Comparator Results Emu UC Davis Feb. 26, 2005 Yangheng Zheng University of California, Los Angeles  Motivation & Introduction.
Christine KOURKOUMELIS University of Athens ATLAS Muon Chamber construction in Greece and alignment studies for H  ZZ  4μ decay Como, 8/10/03.
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.
The first testing of the CERC and PCB Version II with cosmic rays Catherine Fry Imperial College London CALICE Meeting, CERN 28 th – 29 th June 2004 Prototype.
1 Cluster Quality in Track Fitting for the ATLAS CSC Detector David Primor 1, Nir Amram 1, Erez Etzion 1, Giora Mikenberg 2, Hagit Messer 1 1. Tel Aviv.
Yiftah Silver Tel Aviv University September 27 th 2012.
2012 IEEE Nuclear Science Symposium Anaheim, California S. Colafranceschi (CERN) and M. Hohlmann (Florida Institute of Technology) (for the CMS GEM Collaboration)
Muon System and Physics Performance Ludovico Pontecorvo CERN-INFN.
14/02/2007 Paolo Walter Cattaneo 1 1.Trigger analysis 2.Muon rate 3.Q distribution 4.Baseline 5.Pulse shape 6.Z measurement 7.Att measurement OUTLINE.
Precision Drift Chambers for the ATLAS Muon Spectrometer Susanne Mohrdieck Max-Planck-Institut f. Physik, Munich for the ATLAS Muon Collaboration Abstracts:
Updates on GEMs characterization with APV electronics K. Gnanvo, N. Liyanage, K. Saenboonruang.
Brookhaven Science Associates U.S. Department of Energy 1 LECC2005 Advanced Front End Signal Processing Electronics for ATLAS CSC System: Status and post.
Konstantinos Nikolopoulos University of Athens / BNL ATLAS Cathode Strip Chambers Installation and Commissioning XXVI Workshop on Recent Developments in.
Chevron / Zigzag Pad Designs for Gas Trackers
Muon Detector Jiawen ZHANG Introduction The Detector Choices Simulation The structure and detector design The Expected performance Schedule.
Yosuke Watanabe….. University of Tokyo, RIKEN A, KEK C, Development of a GEM tracker for E16 J-PARC 1 Thanks to ???????????
QGP France sept 2010Sanjoy Pal Performances of the tracking Chambers of the ALICE MUON Spectrometer 1.
Yiftah Silver Tel Aviv University September 27 th 2012.
Performance of a Large-Area GEM Detector Prototype for the Upgrade of the CMS Muon Endcap System Vallary Bhopatkar M. Hohlmann, M. Phipps, J. Twigger,
1 A.Andronic 1, H.Appelshäuser 1, V.Babkin 2, P.Braun-Munzinger 1, S.Chernenko 2, D.Emschernmann 3, C.Garabatos 1, V.Golovatyuk 2, J.Hehner 1, M.Hoppe.
June 22, 2009 P. Colas - Analysis meeting 1 D. Attié, P. Colas, M. Dixit, Yun-Ha Shin (Carleton and Saclay) Analysis of Micromegas Large Prototype data.
A Study of Proton-Proton Collisions at the LHC The Ohio State University - Task A.2 B.G. Bylsma, L.S. Durkin, D. Fisher, J Gilmore, J.H. Gu, D. Larson,
M. Bianco On behalf of the ATLAS Collaboration
Shashlyk FE-DAQ requirements Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group PANDA FE-DAQ workshop, Bodenmais April 2009.
GEM basic test and R&D plan Takuya Yamamoto ( Saga Univ. )
Luca Spogli Università Roma Tre & INFN Roma Tre
Mariana Petris, NIPNE Bucharest CBM Meeting, March 9 -12, 2005 HIGH COUNTING RATE TRANSITION RADIATION DETECTOR Bucharest Prototype In Beam Tests.
Studying the efficiency and the space resolution of resistive strips MicroMegas Marco Villa – CERN MAMMA meeting Tuesday, 13 th December 2011 CERN, Geneva.
Calibration of the gain and measurement of the noise for the apv25 electronics K. Gnanvo, N. Liyanage, C.Gu, K. Saenboonruang From INFN Italy: E. Cisbani,
The experimental setup of Test Beam HE EE ES BEAM  A slice of the CMS calorimter was tested during summer of 2007 at the H2 test beam area at CERN with.
June 6, 2001 Paul O’Connor, BNL ATLAS Cathode Strip Chambers.
Precision Drift Chambers for the ATLAS Muon Spectrometer
CALICE Tungsten HCAL Prototype status Erika Garutti Wolfgang Klempt Erik van der Kraaij CERN LCD International Workshop on Linear Colliders 2010, October.
R&D for Muon Trigger Upgrade Naohito Saito (Kyoto/RIKEN/RBRC)
2002 LHC days in Split Sandra Horvat 08 – 12 October, Ruđer Bošković Institute, Zagreb Max-Planck-Institute for Physics, Munich Potential is here...
Proportional chambers with cathode readout in high particle flux environment Michał Dziewiecki.
An electron/positron energy monitor based on synchrotron radiation. I.Meshkov, T. Mamedov, E. Syresin, An electron/positron energy monitor based on synchrotron.
meeting, Oct. 1 st 2015 meeting, Oct. 1 st Gas Pixel: TRD + Tracker.
1 First Results of the SLD Cerenkov Polarimeter at the DESY test beam Oleg Eyser Daniela K äfer, Christian Helebrant, Jenny List, Ulrich Velte*
DHCAL Jan Blaha R&D is in framework of the CALICE collaboration CLIC08 Workshop CERN, 14 – 17 October 2008.
A. SarratILC TPC meeting, DESY, 15/02/06 Simulation Of a TPC For T2K Near Detector Using Geant 4 Antony Sarrat CEA Saclay, Dapnia.
Testbeam analysis Lesya Shchutska. 2 beam telescope ECAL trigger  Prototype: short bars (3×7.35×114 mm 3 ), W absorber, 21 layer, 18 X 0  Readout: Signal.
Siena, May A.Tonazzo –Performance of ATLAS MDT chambers /1 Performance of BIL tracking chambers for the ATLAS muon spectrometer A.Baroncelli,
FEE for Muon System (Range System) Status & Plans G.Alexeev on behalf of Dubna group Turin, 16 June, 2009.
Precision Drift Tube Detectors for High Counting Rates O. Kortner, H. Kroha, F. Legger, R. Richter Max-Planck-Institut für Physik, Munich, Germany A. Engl,
MICROMEGAS per l’upgrade delle Muon Chambers di ATLAS per SLHC Arizona, Athens (U, NTU, Demokritos), Brookhaven, CERN, Harvard, Istanbul (Bogaziçi, Doğuş),
Beam test of Silicon-Tungsten Calorimeter Prototype
MDT second coordinate readout: status and perspectives
CMS muon detectors and muon system performance
Panagiotis Kokkas Univ. of Ioannina
Detection of muons at 150 GeV/c with a CMS Preshower Prototype
Setup for measurements with SCT128 in Ljubljana: SCTA128VG chip
PHENIX RPC R&D EFFORT Beau Meredith
5% The CMS all silicon tracker simulation
Use of Beam Loss Monitor type detectors in CNGS muon station
Status of muon monitor R&D and construction
High Rate Photon Irradiation Test with an 8-Plane TRT Sector Prototype
GEANT Simulations and Track Reconstruction
Pre-installation Tests of the LHCb Muon Chambers
11th Pisa meeting on advanced detectors
Engineering Design Review
Presentation transcript:

CSC Test Beam Data Analysis Alexander Khodinov and Valeri Tcherniatine

Outline  Cathode Strip Chambers in ALTAS  CSC Principle of Operation  CSC Beam Test Layout at X5 (stand alone experiment, CERN)  CSC position resolution and inefficiency

ATLAS Cathode Strip Chambers CSC Electronics:  24,576 Precision Channels (X)  6,144 Transverse Channels (Y)  256 – 96 channel ASM1 (X) Boards  64 – 96 channel ASM1 (Y) Boards  160 – 192 channel ASM2 Boards 2x16 chambers

ATLAS Muon Spectrometer  =2.7

Principle of Operation  Determine muon position by interpolating the charge on 3 to 5 adjacent strips using ratio algorithm:  Precision (x-) strip pitch ~ 5mm  Measure Q 1, Q 2, Q 3 … with signal/noise=150/1  to get  x ~  m. Human hire diameter ~100  m.  Second set of y-strips measure transverse coordinate to ~ 1 cm.  Position accuracy unaffected by gas gain or drift time variations. S = d = 2.50 mm W = mm 0.8Ar+0.2CO 2

Beam test setup layout at X5 high radiation facility P  =120 GeV/C Lead absorbers of different thicknesses were used to vary the background flux intensity. ←

On-line event viewer by M. Schernau

Signal shape and fitting The bipolar function was used to fit the signal: z = (t-t 0 )/  n=12 - the parameter of amplifier integration, t 0 - signal start position  - signal width signal has been digitized at 20(40)MHz Clock time distance between time slices 50(25)ns pedestal extracted

Beam profile distributions

Landau distribution Charge induced in ADC counts: Q = Q max +Q right +Q left

Position resolution and inefficiency Inefficiency: Position resolution in 2 nd and 3 rd gaps defined as (two chambers involved), where  - width of the Gaussian fit of    over ±0.3mm

CSC one layer resolution and inefficiency as a function of background radiation rate Run 99 Run04

Summary stand alone test beam at X5  During the beam test the chamber + electronics at 20 MHz clock showed the expected performance.  One layer inefficiency is found to be 5% without radiation and 24% at the maximal expected LHC background rate (safety factor of 5) 4.2 kHz/cm 2  No calibration used. The results can be considered as conservative estimates (not worse then) for efficiency and resolution.