First steps on optimising RICH analysis

Slides:



Advertisements
Similar presentations
CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
Advertisements

Proposal for a new design of LumiCal R. Ingbir, P. Ruzicka, V. Vrba October 07 Malá Skála.
Update on diffuse extraterrestrial neutrino flux search with 2000 AMANDA-II data Jessica Hodges, Gary Hill, Jodi Cooley This version of the presentation.
E/π identification and position resolution of high granularity single sided TRD prototype M. Târzilă, V. Aprodu, D. Bartoş, A. Bercuci, V. Cătănescu, F.
14 Sept 2004 D.Dedovich Tau041 Measurement of Tau hadronic branching ratios in DELPHI experiment at LEP Dima Dedovich (Dubna) DELPHI Collaboration E.Phys.J.
MDC-II LVL-1 Trigger Khaled Teilab for the MDC Trigger Team.
Veto Wall Test Hyupwoo Lee MINERvA/Jupiter Group Meeting Oct, 3, 2007.
1Calice-UK Cambridge 9/9/05D.R. Ward David Ward Compare Feb’05 DESY data with Geant4 and Geant3 Monte Carlos. Work in progress – no definitive conclusions.
Comparing ZS to VR David Stuart, UC Santa Barbara June 19, 2007.
Cluster Threshold Optimization from TIF data David Stuart, UC Santa Barbara July 26, 2007.
Octal ASD Certification Tests at Michigan J. Chapman, Tiesheng Dai, & Tuan Bui August 30, CERN.
An offline look at TIF data David Stuart UC Santa Barbara May 2, 2007.
1 4 th June 2007 C.P. Ward Update on ZZ->llnunu Analysis and Sensitivity to Anomalous Couplings Tom Barber, Richard Batley, Pat Ward University of Cambridge.
Tests with JT0623 & JT0947 at Indiana University Nagoya PMT database test results for JT0623 at 3220V: This tube has somewhat higher than usual gain. 5×10.
Tracking within hadronic showers in the SDHCAL Imad Laktineh.
Muon alignment with Cosmics: Real and Monte Carlo data S.Vecchi, S.Pozzi INFN Ferrara 37th Software Week CERN June 2009.
Optimising Cuts for HLT George Talbot Supervisor: Stewart Martin-Haugh.
11 Sep 2009Paul Dauncey1 TPAC test beam analysis tasks Paul Dauncey.
Some investigations on Shower in Aug11 DST Szymon Harabasz Version: 15 November 2015.
K  group activities K + K - retracking features New vs Old : resolution future planning. Conclusion and outlook K + K - retracking features New vs Old.
V.Patera – KLOE GM – Otranto – 10 June 2002 K  reconstruction status K + K - retracking features New vs Old : resolution New vs Old : efficiencies Conclusion.
Experimental data by HADES PID method As an example let`s take deuterons and protons with p = 750 MeV/c. Their PDFs are gaussians with mean at β = p/(
Background Subtraction and Likelihood Method of Analysis: First Attempt Jose Benitez 6/26/2006.
1 Performance of a Magnetised Scintillating Detector for a Neutrino Factory Scoping Study Meeting Rutherford Appleton Lab Tuesday 25 th April 2006 M. Ellis.
Normal text - click to edit HLT tracking in TPC Off-line week Gaute Øvrebekk.
Hadron production in C+C at 1 and 2 A GeV analysis of data from experiments NOV02 and AUG04 for high resolution tracking (Runge-Kutta tracks) Pavel Tlustý,
1ECFA/Vienna 16/11/05D.R. Ward David Ward Compare these test beam data with Geant4 and Geant3 Monte Carlos. CALICE has tested an (incomplete) prototype.
Status Report particle identification with the RICH detector Claudia Höhne - GSI Darmstadt, Germany general overview focus on ring radius/ Cherenkov angle.
Min-DHCAL: Measurements with Pions Benjamin Freund and José Repond Argonne National Laboratory CALICE Collaboration Meeting Max-Planck-Institute, Munich.
Detector alignment Stefania and Bepo Martellotti 20/12/10.
D 0 reconstruction: 15 AGeV – 25 AGeV – 35 AGeV M.Deveaux, C.Dritsa, F.Rami IPHC Strasbourg / GSI Darmstadt Outline Motivation Simulation Tools Results.
Estimate of META efficiency in NOV02 Aim: check of META efficiency implemented in digitizers in order to get proper efficiency correction of yields Needed:
1 CPC2-CPR2 Assemblies Testing Status Charge Amplifiers –Attempts to make them work Best voltage single channel 2MHz Cluster finding first.
A Highly Selective Dilepton Trigger System Based on Ring Recognition Alberica Toia II Physikalisches Institut Justus-Liebig-Universität Gießen, Germany.
Update on Diffractive Dijets Hardeep Bansil University of Birmingham 12/07/2013.
January 13, 2004A. Cherlin1 Preliminary results from the 2000 run of CERES on low-mass e + e - pair production in Pb-Au collisions at 158 A GeV A. Cherlin.
Hadron production in C+C at 1 and 2 A GeV analysis of data from experiments NOV02 and AUG04 for high resolution tracking (Runge-Kutta tracks) Pavel Tlustý,
EAS simulated acceptance skymap Olivier Martineau-Huynh 30/04/2014.
Hadron production in C+C at 2 A GeV measured by the HADES spectrometer Nov02 gen3 analysis and results for spline tracks (shown in Dubna) changes - removing.
J.Pietraszko, HADES Coll. Meeting, GSI Nov ,  – electron multiplicity measured in HADES W. Koenig, Jerzy Pietraszko, T. Galatyuk, V. Pechenov,
HADRON 2009, FloridaAnar Rustamov, GSI Darmstadt, Germany 1 Inclusive meson production at 3.5 GeV pp collisions with the HADES spectrometer Anar Rustamov.
Quark Matter 2002, July 18-24, Nantes, France Dimuon Production from Au-Au Collisions at Ming Xiong Liu Los Alamos National Laboratory (for the PHENIX.
Beam detectors in Au+Au run and future developments - Results of Aug 2012 Au+Au test – radiation damage - scCVD diamond detector with strip metalization.
June 4, 2009 STAR TPC review Estimation of TPC Aging Based on dE/dx Measurements Yuri Fisyak.
Multi-lepton and general searches at HERA Andrea Parenti (DESY-Hamburg) on behalf of H1 and ZEUS collaborations - DIS Outline: ● Multi-electron.
IPHC, Strasbourg / GSI, Darmstadt
April12 DST calibration status
A Kalman Filter for HADES
Using IP Chi-Square Probability
RAPID/IES Calibration Status Rutherford Appleton Lab
CluTim Algorithm for Drift Chambers Readout Electronics
Update on Noise Analysis of the DHCal Test Beam at Fermilab
Tracking results from Au+Au test Beam
Shower detector status report
TOF CALIBRATION DATABASE
HARPO Analysis.
Simulation results for the upgraded RICH detector in the HADES experiment. Semen Lebedev1,3, Jürgen Friese2, Claudia Höhne1, Tobias Kunz2, Jochen Markert4.
Noise analysis of the 1m3 DHCal test beam
Status of the "direct" photon reconstruction
Measurement of p0 – induced single leptons in the HADES RICH
Status of the TOF Detector
CLAS12 MesonEx trigger studies
Photon Detection Efficiency in the CsI-based HADES RICH
2000 Diffuse Analysis Jessica Hodges, Gary Hill, Jodi Cooley
Commissioning of the ALICE-PHOS trigger
Jessica Leonard Oct. 23, 2006 Physics 835
Exercises on sheet similar to this
August 19th 2013 Alexandre Camsonne
CLAS Collaboration Meeting
Clustering-based Studies on the upgraded ITS of the Alice Experiment
Presentation transcript:

First steps on optimising RICH analysis Outline: Improved ring-track matching for low momentum (W.Koenig) Pad multiplicity and comparison with simulation Summary and conclusion Christina Dritsa JLU Giessen XXV Hades Collaboration Meeting, GSI. Darmstadt 19-23 November

Improve ring track matching for low momenta W.Koenig

Improve ring track matching for low momenta W.Koenig

Improve ring track matching for low momenta W.Koenig

Improve ring track matching for low momenta W.Koenig

Pad multiplicity and comparison with simulation

RICH analysis - reminder 0. Hardware thresholds (pedestals, cut on 3xσ noise) 1. Cleaning: Removes 2 types of structures single pads (mainly firing due to unusually high noise) large structures with high pulse (from direct hits) 2. Labelling: flag areas to search for rings (increase speed of analysis) 3. Ring finding “Hough” transform Pattern matrix Question: Is there room for optimising these steps to enhance the ring finding efficiency without creating more fake rings?

Pedestals S0 S1 S2 S3 S4 S5 DATA, apr12 SIMULATION, apr12 Uniform distribution of thresholds over all the sector surface Same for simulation

Thresholds S0 S1 S2 S3 S4 S5 DATA, apr12 SIMULATION, apr12 Pattern may be explained by the different lengths of circuit paths connecting the pad and the amplifier. This leads to different capacitances and hence the noise of the channels vary slightly. Middle lines with high thresholds are due to missing CsI cathode coverage at the edges of the 3 sector segments.

RICH “anatomy” http://hades-wiki.gsi.de/pub/RICH/RichFrontEnds/sector.pdf Anton Johann Kastenmüller, PhD thesis

Same effect observed before (old electronics) Anton Johann Kastenmüller, PhD thesis (2000) Note that in simulation the noise is always represented by a Gaussian function. This is not the case in reality: noise distribution has “tails”!

Investigation of the pad multiplicity for different event multiplicity classes

Number of hits ToF+RPC

All firing pads, Sector 0, day 123 0-20 > Slight dependence on event multiplicity. > Inner part of sector has relatively high occupancy > Similar behaviour observed for all sectors 80-100 160-180

Single pads removed, sector 0, day 123 > No dependence on event multiplicity, as expected. > Similar behaviour observed for all sectors (not shown here)

Single pads remaining, sector 0, day 123 Slight dependence on event multiplicity. Inner part of sector has relatively high occupancy Are thresholds lower than needed? Enhancement of fake rings? Similar behaviour observed for all sectors

Comparison to simulation: Number of remaining pads as a function of theta DATA SIMULATION

Comparison to simulation: Number of remaining pads as a function of theta DATA SIMULATION

Comparison to simulation: Number of rings as function of theta Data, all sectors Simulation, all sectors 100k events 60k events Real data are seemingly dominated by high noise in the low theta region. This might lead to fake rings which pass the standard ring quality cuts! Discrepancy with simulation!

Ring-to-proton matching θrich S0 Select protons from ToF/RPC: β<0.7 charge==1 mom>700MeV Select Rings: AC>70 Centr>0 matched ring index Selected rings match to identified protons from ToF/RPC. Clear enhancement of the fake matches in the low theta region (RPC region)

Summary New method introduced by Wolfgang improves ring-track matching for low momentum tracks by a factor up to 6! Non uniform noise levels lead to non-uniform threshold settings: Low theta region seems to have much higher occupancy potentially due to too low threshold settings Problem with “good quality” fake rings matching to non-leptons for low theta Discrepancies between simulation and measurement for pad and ring multiplicities Outlook Need to bring simulation and measurement closer! Investigate different threshold settings (e.g. increase thresholds in inner theta region) Update noise in simulation: Replace Gauss by “Gauss+tails” taken by measurement Investigate close pair rejection (in progress by Wolfgang)

Improve ring track matching for low momenta W.Koenig

Same effect observed before (old electronics) Anton Johann Kastenmüller, PhD thesis (2000) Note that in simulation the noise is always represented by a Gaussian function. This is not the case in reality: noise distribution has “tails”! Effect smoothed out with improved grounding. Measurements done in laboratory with pulser.

close pair investigation W.Koenig