On Noise Characterization Michel Lefebvre University of Victoria Physics and Astronomy 14 August 2003.

Slides:



Advertisements
Similar presentations
ATLAS Tile Calorimeter Performance Henric Wilkens (CERN), on behalf of the ATLAS collaboration.
Advertisements

Giuseppe Roselli (CMS-RPC) Università degli Studi di Bari – INFN RPC Efficiency with Track Reconstruction Giuseppe Roselli.
R. Zitoun, Stony Brook and LAPP CTF Meeting10 February Much Noise About Nothing? Robert Zitoun Stony Brook and LAPP CTF Meeting February 10, 2003.
Digital Filtering Performance in the ATLAS Level-1 Calorimeter Trigger David Hadley on behalf of the ATLAS Collaboration.
S 1 Summer Student Sessions 13 August 2008 Chew Soo Hoon University Of Malaya, Malaysia Jan Stark LPSC, Grenoble, France
TRACK DICTIONARY (UPDATE) RESOLUTION, EFFICIENCY AND L – R AMBIGUITY SOLUTION Claudio Chiri MEG meeting, 21 Jan 2004.
Adding electronic noise and pedestals to the CALICE simulation LCWS 19 – 23 rd April Catherine Fry (working with D Bowerman) Imperial College London.
29 June 2004Paul Dauncey1 ECAL Readout Tests Paul Dauncey For the CALICE-UK electronics group A. Baird, D. Bowerman, P. Dauncey, C. Fry, R. Halsall, M.
M. Lefebvre, 31 May 2006 (updated 2006/06/04)Noise and correlation issues1 Noise and correlation issues using LArNoiseMonToolBase M. Lefebvre University.
M. Lefebvre, 8 June 2006Noise and correlation monitoring1 Noise and correlation monitoring using LArNoiseMonToolBase M. Lefebvre University of Victoria.
Wavelet Transform A very brief look.
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.
Digital Hadron Calorimeter Cosmic Ray Test Stand As of 9am05/12/2003 Note: axes on scatter plots are reversed.
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.
25 July 2005Michel Lefebvre 1 Noise file for EMEC-HEC 2002 data Michel Lefebvre Physics and Astronomy University of Victoria British Columbia, Canada 25.
Top mass in t-tbar  6jets Status Report Physics and Astronomy University of Victoria British Columbia, Canada Top meeting CERN, 21 Feb 2007 Michel Lefebvre.
Event Phase Reconstruction Raw TDC Event time used for monitoring Event phase  TBPhaseRec  TBPhase Michel Lefebvre Rob McPherson University of Victoria.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
Cosmic Ray Test Stand with Scintillating Cells for Digital Hadron Calorimeter As of 9am 05/28/2003.
Digital Hadron Calorimeter Cosmic Ray Test Stand.
M. Lefebvre, 6 June 2006Noise and correlation monitoring1 Noise and correlation monitoring using LArNoiseMonToolBase M. Lefebvre University of Victoria.
Michele Faucci Giannelli TILC09, Tsukuba, 18 April 2009 SiW Electromagnetic Calorimeter Testbeam results.
A VOICE ACTIVITY DETECTOR USING THE CHI-SQUARE TEST
Rate and Gain Measurements of the 1-m long GEM detector Aiwu Zhang EIC tracking R&D weekly meeting.
Development of Readout ASIC for FPCCD Vertex Detector 01 October 2009 Kennosuke.Itagaki Tohoku University.
Performance of SPIROC chips in SKIROC mode
The Transverse detector is made of an array of 256 scintillating fibers coupled to Avalanche PhotoDiodes (APD). The small size of the fibers (5X5mm) results.
SSD Status P. Christakoglou (NIKHEF-UU) for the SSD collaboration Thanks to: Marco vL, Enrico, Mino, Marek and Massimo.
The Wavelet Tutorial: Part3 The Discrete Wavelet Transform
Dr. Richard Young Optronic Laboratories, Inc..  Uncertainty budgets are a growing requirement of measurements.  Multiple measurements are generally.
On The Geometry of the HEC Readout Channels Local HEC coordinate system Readout families Readout channels Volumes and geometrical centers Neighbors Michel.
On The Geometry of the EMEC Readout Channels
W  eν The W->eν analysis is a phi uniformity calibration, and only yields relative calibration constants. This means that all of the α’s in a given eta.
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.
ATLAS Liquid Argon Calorimeter Monitoring & Data Quality Jessica Levêque Centre de Physique des Particules de Marseille ATLAS Liquid Argon Calorimeter.
ECFA Sep 2004Paul Dauncey - CALICE Readout1 CALICE ECAL Readout Status Paul Dauncey For the CALICE-UK electronics group A. Baird, D. Bowerman, P.
A. Gibson, Toronto; Villa Olmo 2009; ATLAS LAr Commissioning October 5, 2009 Commissioning of the ATLAS Liquid Argon Calorimeter Adam Gibson University.
Combined HEC/EMEC testbeam data can be read and analyzed within the ATLAS Athena framework A “cookbook” gives an introduction for how to access the data.
EXAMINATION OF CORRUPTED DATA IN THE TILE CALORIMETER Stephanie Hamilton Michigan State University The ATLAS Collaboration Supervisor: Irene Vichou (U.
1 Calice UK Meeting 27/03/07David Ward Plans; timescales for having analysis results for LCWS Status of current MC/data reconstruction Reconstruction status;
HBD FEE test result summary + production schedule 16mv test pulse result –5X attenuator + 20:1 resistor divider at input (to reduce the noise on the test.
23 November Md. Tanvir Al Amin (Presenter) Anupam Bhattacharjee Department of Computer Science and Engineering,
Dec.11, 2008 ECL parallel session, Super B1 Results of the run with the new electronics A.Kuzmin, Yu.Usov, V.Shebalin, B.Shwartz 1.New electronics configuration.
16-Nov-2002Konstantin Beloous1 Digital Hadron Calorimeter Energy Resolution.
18/01/01GEO data analysis meeting, Golm Issues in GW bursts Detection Soumya D. Mohanty AEI Outline of the talk Transient Tests (Transient=Burst) Establishing.
January 21, 2007Suvadeep Bose / IndiaCMS - Santiniketan 1 Response of CMS Hadron Calorimeter to Electron Beams Suvadeep Bose EHEP, TIFR, Mumbai Outline:
Study of neutrino oscillations with ANTARES J. Brunner.
Results from particle beam tests of the ATLAS liquid argon endcap calorimeters Beam test setup Signal reconstruction Response to electrons  Electromagnetic.
Digital Processing for EELS Data Xiang Yang WATLABS, Univeristy of Waterloo.
S.MonteilCaloPiquet1 August 2010 – A typical online Calo Piquet Analysis - Outline of the analysis (Fill 1264 – Run #77195) 1. Calorimeter 2DViews, inclusive.
12 October 2001, M. LefebvreHEC-Athena Tutorial: HEC beam test primer1 HEC Beam Test Primer Production modules of the HEC have been tested in particle.
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,
CALOR April Algorithms for the DØ Calorimeter Sophie Trincaz-Duvoid LPNHE – PARIS VI for the DØ collaboration  Calorimeter short description.
CGH Data BIOS Chromosome Re-arrangements.
Calice Meeting Argonne Muon identification with the hadron calorimeter Nicola D’Ascenzo.
Analysis for QA (temporary) Hideyuki Sakamoto 1 st October 2007 MICE Tracker Phone Meeting.
1 M2-M5 Efficiency and Timing checks on 7TeV beam data Alessia, Roberta R.Santacesaria, April 23 rd, Muon Operation
Lucia Bortko | Optimisation Studies for the BeamCal Design | | IFJ PAN Krakow | Page 1/16 Optimisation Studies for the BeamCal Design Lucia.
M. LefebvreATLAS LAr week, November 19th HEC-EMEC beam test data analysis Filtering weight synchronization and timing issues TDC timing Cubic timing.
The ATLAS Electromagnetic and Hadronic End-Cap Calorimeter in a Combined Beam Test Tamara Hughes University of Victoria WRNPPC 2004.
G. Eigen, Paris, Introduction The SiPM response is non-linear and depends on operating voltage (V-V bd ) and temperature  SiPMs need monitoring.
Comparison of MC and data Abelardo Moralejo Padova.
Sensitivity of HO to Muons Shashi Dugad for HO group India-CMS Meeting 6-7 Oct
CluTim Algorithm for Drift Chambers Readout Electronics
Analysis of FADC single-crystal data
IX International Workshop ACAT
Image filtering Images by Pawan Sinha.
1) Adding new ions into PIKA to account for
Image filtering Images by Pawan Sinha.
DESY drift chambers efficiency and track reconstruction
Presentation transcript:

On Noise Characterization Michel Lefebvre University of Victoria Physics and Astronomy 14 August 2003

M. Lefebvre, 14 August 2003On Noise Characterization2 Noise Characterization A good characterization of the digital filtering noise is crucial to most analysis The digital filtering noise reduction factor depends on the layer and on  Strategy to estimate the digital filtering noise for each channel using only a given data run:  The pedrms are obtained from the first time sample the usual way;  For the channels with no signal in them (following some criteria), compute the noise/pedrms, where the noise is the result of a gaussian fit;  Obtain the average noise/pedrms ratio for a given layer and  ;  Interpolate to other channels (those considered to have signal in them) using the corresponding average noise/pedrms ratio;  This is implemented in TBRootAna as NoiseAlg.

M. Lefebvre, 14 August 2003On Noise Characterization3 Noise Characterization: HEC The digital filtering noise reduction factor depends on the layer and on  and ranges from 0.54 to 0.70  noise/pedrms  vs  noise vs  is a muon run

M. Lefebvre, 14 August 2003On Noise Characterization4 Noise Characterization: EMEC The digital filtering noise reduction factor depends on the layer and on  and ranges from 0.46 to 0.77  noise/pedrms  vs  noise vs  is a muon run

M. Lefebvre, 14 August 2003On Noise Characterization5 Occupancy Consider the occupancy of all cells for a given run, obtained using pedrms as a noise characterization occupancy computed using |signal| > 1pedrms expect channels with no signal to be at 31.7%. They are not! the occupancy distribution is broad because the noise/pedrms ratio varies over the calorimeters the number of entries in each plot is the number of connected readout channels for each detector is a muon run HEC EMEC a few dead channels

M. Lefebvre, 14 August 2003On Noise Characterization6 Noise Quality The quality of the digital filtering noise can be assessed by studying the occupancy of all cells for a given run occupancy computed using |signal| > 2  expect channels with no signal to be at 4.55%. They are! Their distribution is narrow channels with signal in them clearly have large occupancy (here only a few since this is a muon run) There are a few very noisy channels with non-gaussian noise (next slide) the number of entries in each plot is the number of connected readout channels for each detector is a muon run HEC EMEC a few dead channels

M. Lefebvre, 14 August 2003On Noise Characterization7 Pathological Channels Some very noisy channels have non-gaussian digital filtering noise distribution  Their pedestal distribution is gaussian;  The non-gaussian nature of the noise distribution seems to be generated by the digital filtering reconstruction  A limited range gaussian fit underestimates the noise, and hence overestimates the occupancy  They obviously need special treatment...  Seems to be limited to some EMEC channels in layers 1 and 2 run Kanaya Ch1024 pedrms Ch1024 noise