1 MDT P ERFORMANCE WITH 2012 C OLLISION D ATA C ONTENT OF THE CONF-NOTE Mauro Iodice Muon Week – Muon Performance Meeting, May 15 th, 2013.

Slides:



Advertisements
Similar presentations
Giuseppe Roselli (CMS-RPC) Università degli Studi di Bari – INFN RPC Efficiency with Track Reconstruction Giuseppe Roselli.
Advertisements

Muon Data Quality and Performance A. Belloni - G. Zevi Della Porta for the ATLAS Harvard Group DOE Site Visit
May 14, 2015Pavel Řezníček, IPNP Charles University, Prague1 Tests of ATLAS strip detector modules: beam, source, G4 simulations.
TRACK DICTIONARY (UPDATE) RESOLUTION, EFFICIENCY AND L – R AMBIGUITY SOLUTION Claudio Chiri MEG meeting, 21 Jan 2004.
CMS Physics Meeting, Dec. 6, Analysis Note on the Validation of the ORCA Simulation of the Endcap Muon CSC Front-end Electronics S. Durkin -- Ohio.
D. Peterson, Muon Spectrometers at ATLAS and CMS, presentation to LEPP 19-Nov  spectrometers at ATLAS and CMS Our charge: Survivability Resolution.
Measurement of B (D + →μ + ν μ ) and the Pseudoscalar Decay Constant f D at CLEO István Dankó Rensselaer Polytechnic Institute representing the CLEO Collaboration.
MCP checks for the H-4l mass. Outline and work program The problems: – Higgs mass difference from the  – Possible single resonant peak mass shift (with.
PERFORMANCE OF THE MACRO LIMITED STREAMER TUBES IN DRIFT MODE FOR MEASUREMENTS OF MUON ENERGY - Use of the MACRO limited streamer tubes in drift mode -Use.
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
NSW background studies Max Bellomo, Nektarios Benekos, Niels van Eldik, Andrew Haas, Peter Kluit, Jochen Meyer, Felix Rauscher 1.
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.
MdcPatRec Tracking Status Zhang Yao, Zhang Xueyao Shandong University.
25/07/2002G.Unal, ICHEP02 Amsterdam1 Final measurement of  ’/  by NA48 Direct CP violation in neutral kaon decays History of the  ’/  measurement by.
Precision Drift Chambers for the ATLAS Muon Spectrometer Susanne Mohrdieck Max-Planck-Institut f. Physik, Munich for the ATLAS Muon Collaboration Abstracts:
Status of straw-tube tracker V.Peshekhonov, D.Peshekhonov, A.Zinchenko JINR, Dubna V.Tikhomirov P.N.Lebedev Physics Institute, Moscow Presented on the.
HERA-LHC, CERN Oct Preliminary study of Z+b in ATLAS /1 A preliminary study of Z+b production in ATLAS The D0 measurement of  (Z+b)/  (Z+jet)
Calibration of the CMS Electromagnetic Calorimeter with first LHC data
Muon-raying the ATLAS Detector
Simonetta Gentile, LCWS10, March 2010, Beijing,China. G-APD Photon detection efficiency Simonetta Gentile 1 F.Meddi 1 E.Kuznetsova 2 [1]Università.
1 Energy loss correction for a crystal calorimeter He Miao Institute of High Energy Physics Beijing, P.R.China.
Simulation of Beam-Beam Background at CLIC André Sailer (CERN-PH-LCD, HU Berlin) LCWS2010: BDS+MDI Joint Session 29 March, 2010, Beijing 1.
Mitglied der Helmholtz-Gemeinschaft Calibration of the COSY-TOF STT & pp Elastic Analysis Sedigheh Jowzaee IKP Group Talk 11 July 2013.
21 Jun 2010Paul Dauncey1 First look at FNAL tracking chamber alignment Paul Dauncey, with lots of help from Daniel and Angela.
CMS WEEK – MARCH06 REVIEW OF MB4 COMMISSIONING DATA Giorgia Mila
Luca Spogli Università Roma Tre & INFN Roma Tre
Results from particle beam tests of the ATLAS liquid argon endcap calorimeters Beam test setup Signal reconstruction Response to electrons  Electromagnetic.
A. Meneguzzo Padova University & INFN Validation and Performance of the CMS Barrel Muon Drift Chambers with Cosmic Rays A. Meneguzzo Padova University.
1 A first look at the KEK tracker data with G4MICE Malcolm Ellis 2 nd December 2005.
Particle Identification at BESIII Kanglin He April 23, 2007, Amsterdam.
Preliminary results for the BR(K S  M. Martini and S. Miscetti.
Test beam preliminary results D. Di Filippo, P. Massarotti, T. Spadaro.
Progress on F  with the KLOE experiment (untagged) Federico Nguyen Università Roma TRE February 27 th 2006.
Precision Drift Chambers for the ATLAS Muon Spectrometer
PERFORMANCE OF THE PHENIX SOUTH MUON ARM Kenneth F. Read Oak Ridge National Lab & University of Tennessee for the PHENIX Collaboration Quark Matter 2002.
Measurement of the Charge Ratio of Cosmic Muons using CMS Data M. Aldaya, P. García-Abia (CIEMAT-Madrid) On behalf of the CMS Collaboration Sector 10 Sector.
1 DT Local Reconstruction on CRAFT data Plots for approval CMS- Run meeting, 26/6/09 U.Gasparini, INFN & Univ.Padova on behalf of DT community [ n.b.:
Notes in preparation by the Torino group Sara BolognesiDT Cosmic Meeting 01/11/2007  MTCC note:  calibration section  DQM section  Internal note about.
Muons at CalDet Introduction Track Finder Package ADC Corrections Drift Points Path Length Attenuation Strip-to-Strip Calibration Scintillator Response.
4/12/05 -Xiaojian Zhang, 1 UIUC paper review Introduction to Bc Event selection The blind analysis The final result The systematic error.
A High Statistics Study of the Decay M. Fujikawa for the Belle Collaboration Outline 1.Introduction 2.Experiment Belle detector 3.Analysis Event selection.
Penny Kasper Fermilab Heavy Quarkonium Workshop 21 June Upsilon production DØ Penny Kasper Fermilab (DØ collaboration) 29 June 2006 Heavy Quarkonium.
06/2006I.Larin PrimEx Collaboration meeting  0 analysis.
Tuning of trigger simulation parameters (Bossi, Moulson, Palutan, Sciascia) Calorimeter trigger thresholds calibration using prompt photons from K S 
Study of 1D Hit Error Assignment Marco Terranova, Filippo Pisano, N. Amapane, G. Cerminara.
Giuseppe Ruggiero CERN Straw Chamber WG meeting 07/02/2011 Spectrometer Reconstruction: Pattern recognition and Efficiency 07/02/ G.Ruggiero - Spectrometer.
Paolo Massarotti Kaon meeting March 2007  ±  X    X  Time measurement use neutral vertex only in order to obtain a completely independent.
Siena, May A.Tonazzo –Performance of ATLAS MDT chambers /1 Performance of BIL tracking chambers for the ATLAS muon spectrometer A.Baroncelli,
Outline Description of the experimental setup Aim of this work TDC spectra analysis Tracking method steps Autocalibration Single tube resolution Summary.
14/02/2008 Michele Bianco 1 G.Chiodini & E.Gorini ATLAS RPC certification with cosmic rays Università del Salento Facoltà di Scienze MM.FF.NN.
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,
Upsilon production and μ-tagged jets in DØ Horst D. Wahl Florida State University (DØ collaboration) 29 April 2005 DIS April to 1 May 2005 Madison.
June 4, 2009 STAR TPC review Estimation of TPC Aging Based on dE/dx Measurements Yuri Fisyak.
Comparison of algorithms for hit reconstruction in the DTs: Test of calibration procedures for t trig and drift velocity on Test Beam data Test of calibration.
First results from prototype measurements
FURTHER STUDIES ON COMMISSIONING DATA
Tracking results from Au+Au test Beam
Results of dN/dt Elastic
Integration and alignment of ATLAS SCT
DT Local Reconstruction on CRAFT data
5% The CMS all silicon tracker simulation
J/: towards first physics results/first paper
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
Quarkonium production in ALICE
STAR Detector Event selection and triggers Corrections to data
Bringing the ATLAS Muon Spectrometer to Life with Cosmic Rays
J/   analysis: results for ICHEP
Problems with the Run4 Preliminary Phi->KK Analysis
Contents First section: pion and proton misidentification probabilities as Loose or Tight Muons. Measurements using Jet-triggered data (from run).
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
Presentation transcript:

1 MDT P ERFORMANCE WITH 2012 C OLLISION D ATA C ONTENT OF THE CONF-NOTE Mauro Iodice Muon Week – Muon Performance Meeting, May 15 th, 2013

2 I NTRODUCTION Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013 Writing/Finalizing THREE CONF-NOTES is one of the short term objectives of the Muon Analysis Task Force (MATF) Working group: -- Alignment CONF-NOTE (main results presented in several talks by Pierre-Francoise) -- MDT Calibrations CONF-NOTE (previous talk by Mike/Ed) -- MDT Performance with collision data CONF-NOTE, mainly focusing on:  Resolution  Efficiencies  Dependence with background hit rates In the following: -- list of content and main results for the MDT Performance CONF-Note Most of the material from recent analyses by Xin Fang MANY THANKS !

3 Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013 MDT P ERFORMANCE C ONF N OTE – P ROPOSED L IST OF C ONTENT 1.MDT tube hit rate Vs Luminosity -- Tube average hit rates per chamber Vs Luminosity -- Saturation effects at high rates ??? (see P.Fleischmann Muon Week March 26 th ) 2.MDT Resolution Vs Drift Radius -- Tube hit Residuals: Establish fitting procedure -- Resolution: Definition and methods -- Resolution measurement for different types of chambers -- Comparison among different methods -- Comparison of results with different track pT selection: check results with curved segments fits at low pT -- Dependence with tube hit rates 3.Efficiencies -- Definition (Hardware efficiency / segment reconstruction efficiency) -- Efficiencies Vs radius for different types of chambers -- Dependence with tube hit rate 1.Comparison with simulation (if available/feasible) starting project on possible aging effects of MDT tubes Vs Integrated luminosity from MDT charge response (ADC) of the tubes Vs time (and Vs position, i.e. occupancy

4 MDT H IT R ATES (H Z / TUBE ) Compute average tube hit rate per chamber counting “out of time” hits in TDC spectra per chamber (and divide by num. tubes)  Hz/tube TDC Barrel A TDC Endcap A Highest rates on EIL1 chambers 37.5 KHz/tube Highest rates on EIL1 chambers 37.5 KHz/tube ~ cm -2 s -1 For ~ cm -2 s -1 Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

5 Average rate per tube per chamber normalized to average tube length x 3cm  Hz/cm 2 Average rate per tube per chamber normalized to average tube length x 3cm  Hz/cm 2 Highest rates on EIL/S chambers ~ 44 Hz/cm 2 Highest rates on EIL/S chambers ~ 44 Hz/cm 2 ~ cm -2 s -1 MDT H IT R ATES N ORMALIZED TO U NIT AREA (H Z /cm 2 ) Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

6 MDT R ESOLUTION V S D RIFT R ADIUS 1. MDT Resolution can be obtained by straight track fitting (segment) from “residual widths”  (r) and extrapolation errors: 1. Can also be obtained by the geometric mean of biased and unbiased hit “residual widths” ( NIM A538 (2005) )  Residual distribution  establish fitting function  Define “residual width” Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

7 MDT R ESOLUTION – F ITTING OF R ESIDUALS Non gaussian shape close to the wire Fit at different radii with Double Gaussian (small contribution from non-core gaussian for r>2mm) Residual Width = weighted average of large and narrow gaussians widths: Resolution estimate insensitive to Systematic offset Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

8 MDT R ESOLUTION – R ESULTS Barrel ABarrel C Endcap AEndcap C Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

9 MDT R ESOLUTION – R ESULTS Provided we accept the fitting procedure and methods, this is now an established results. Many cross-checks performed (can be reported in the CONF-NOTE) All results are consitent Comparison with H8 Test-Beam data – CAVEAT: Test Beam data taken at fixed angles – better knowledge of extrapolation error Test-Beam results obtained with different residual fitting procedure ATLAS Collision data include slewing corrections (not included in TB) Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

10 MDT R ESOLUTION – D EPENDENCE ON H IT R ATE The data-sample was analysed in separate “regions” with increasing luminosities Resolutions for the EIL1 chambers have been estimated (next slides) Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

11 EIL1 R ESOLUTION – R DIFFERENT L UMINOSITIES REGION A Region A ~ cm -2 s -1 Region B ~ cm -2 s -1 Region D ~ cm -2 s -1 Region C ~ cm -2 s -1 NO EVIDENCE OF RESOLUTION DEGRADATION UP TO cm -2 s -1 (~55 Hz/cm 2 ) Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

12 R ESOLUTION D EGRADATION FOR H IGH R ATES …as expected from Test-Beam under high background rates By S.ZIMMERMANN March 2004 (GIF) Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

13 MDT TUBE EFFICIENCY Definition, method, results in “low background rate” reported many times (see e.g. Xin at Muon Week March 26 th ) In the following, the dependence with background hit rate is reported  next slide An example for Barrel A chambers Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

14 EIL1 E FFICIENCY – R DIFFERENT L UMINOSITIES Region A ~ cm -2 s -1 Region B ~ cm -2 s -1 Region D ~ cm -2 s -1 Region C ~ cm -2 s -1 A DROP IN EFFICIENCY of about 3% is observed from to From 20 to 50 kHz/tube

E FFICIENCY DROP WITH T UBE H IT R ATE Good agreement with extrapolated efficiency from tube hit rates and a ~750 ns dead-time after each hit Measured Extrapolation with tube hit rate Mauro Iodice – Muon Week – Performance Meeting, May 15 th, 2013

16 S UMMARY Results on MDT performance studies with 2012 data mature for a CONF-Note Background hit rates: need re-analyses on different runs/Lumi (easy) Resolution studies: -- Procedure established -- Resolution measured with two methods agree -- No degradation of resolution observed up to a tube hit rate of ~55 Hz/cm 2 (as expected) Efficiency studies: -- Procedure established -- Drop in efficiency observed in the Endcap Inner chambers (mainly EIL1 – following the expectations) -- Map of efficiencies per chambers to be done Comparison with simulations: -- Not started yet. Need to check available data sample quality/feasibility/reliability