ITTF “Re-View” Session, August 11, 2003 Manuel Calderón de la Barca Sánchez ITTF Evaluation for Spectra.

Slides:



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

III Convegno sulla Fisica di ALICE. Frascati 1 Vertex reconstruction and selection strategies for D s detection in Pb-Pb collisions Sergey Senyukov,
June 6 th, 2011 N. Cartiglia 1 “Measurement of the pp inelastic cross section using pile-up events with the CMS detector” How to use pile-up.
Final state study Jaewon Park University of Rochester Vittorio Paolone University of Pittsburgh MINERvA Collaboration Meeting, Sep 13-15, 2007.
CC analysis progress This talk: –A first attempt at calculating CC energy sensitivity using the Far Mock data MC files with full reconstruction. –Quite.
Status of  b Scan Jianchun Wang Syracuse University Representing L b scanners CLEO Meeting 05/11/02.
With larger statistics, explore nature of tracks that 1)Are found by Xkal but missed by TRTSeeded 2)Are found by TRTSeeded but missed by Xkal Here are.
Increasing Field Integral between Velo and TT S. Blusk Sept 02, 2009 SU Group Meeting.
Topological D-meson Reconstruction with STAR Using the Silicon Vertex Tracker (SVT) Sarah LaPointe Wayne State University SVT review, BNL, July 7 th /8.
STAR Collaboration Meeting, Nantes, July2002 SVT Analysis/Status Update Jun Takahashi – University of Sao Paulo.
FTPC calibration status Joern Putschke for the STAR FTPC group STAR Analysis Meeting 2002 October 22-24, 2002.
L3 Muon Trigger at D0 Status Report Thomas Hebbeker for Martin Wegner, RWTH Aachen, April 2002 The D0 muon system Functionality of the L3 muon trigger.
Current Status of Hadron Analysis Introduction Hadron PID by PHENIX-TOF  Current status of charged hadron PID  CGL and track projection point on TOF.
Non-identified Two Particle Correlations from Run I Understanding drift chamber tracking – Tracker and candidatory – Two particle efficiencies/ghosts A.
 Production at forward Rapidity in d+Au Collisions at 200 GeV The STAR Forward TPCs Lambda Reconstruction Lambda Spectra & Yields Centrality Dependence.
HADES coll. meeting, Oct. 31, 2007 Charged pion production in C+C at 1 and 2 A GeV results of data analysis from experiments NOV02 and AUG04 Jehad Mousa.
Track extrapolation to TOF with Kalman filter F. Pierella for the TOF-Offline Group INFN & Bologna University PPR Meeting, January 2003.
1 Calorimeter in G4MICE Berkeley 10 Feb 2005 Rikard Sandström Geneva University.
ITTF Status STAR Analysis Meeting Dec 5, 04 Claude Pruneau Wayne State University.
7 May 2009Paul Dauncey1 Tracker alignment issues Paul Dauncey.
First Look at Data and MC Comparisons for Cedar and Birch ● Comparisons of physics quantities for CC events with permutations of Cedar, Birch, Data and.
Integrated Tracker (progress, status, plans) Y. Fisyak.
Update on BES light nuclei w.j. llope I Analysis Mtg, 7/16/2013, Purdue physics directions:
“Vertexig and tracking ” Entirely based on works and results by: S. Rossegger, R. Shahoyan, A. Mastroserio, C. Terrevoli Outline: Comparison Fast simulation.
 0  5  Outline Event selection & analysis Background rejection Efficiencies Mass spectrum Comparison data-MC Branching ratio evaluation Systematics.
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,
FTPC status and results Summary of last data taken AuAu and dAu calibration : Data Quality Physic results with AuAu data –Spectra –Flow Physic results.
W/Z Plan For Winter Conferences Tom Diehl Saclay 12/2001.
Preliminary results for the BR(K S  M. Martini and S. Miscetti.
Z, W bosons: well calibrated probe in pp LHC energies: access to Z, W in pA and AA Electroweak bosons in dilepton channel: No final state modification.
Status of the hadronic cross section (small angle) Federico Nguyen February 22 nd 2005  the 2002 data sample and available MC sets  trigger efficiency.
Current Analysis Activity/Results (Only brief overview) Sunil Bansal (Panjab University, Chandigarh) Approved results marked.
1 Guannan Xie Nuclear Modification Factor of D 0 Mesons in Au+Au Collisions at √s NN = 200 GeV Lawrence Berkeley National Laboratory University of Science.
Samir Guragain, Marcus Hohlmann Florida Institute of Technology, Melbourne, FL Z′ Mass Reach MC Analysis USCMS meeting Brown University May 6 – 8, 2010.
22 January 2009 David1 Look at dead material and fake MET in Jx samples mc08 10 TeV simulations, release J0 to J6 are tag s479_r586, ‘ideal geometry’
Light Nuclei Spectra in STAR Run5 62GeV Cu+Cu Experiments Jianhang Zhou Rice University.
4/12/05 -Xiaojian Zhang, 1 UIUC paper review Introduction to Bc Event selection The blind analysis The final result The systematic error.
Tomas Hreus, Pascal Vanlaer Overview: K0s correction stability tests Jet-pt correction closure test Study of Strangeness Production in Underlying Event.
Tuning of trigger simulation parameters (Bossi, Moulson, Palutan, Sciascia) Calorimeter trigger thresholds calibration using prompt photons from K S 
David Silvermyr Lund University for the PHENIX Collaboration Early global event results using the PHENIX Pad Chambers at RHIC.
Mid-rapidity pi0 production in pp collisions at sqrt(s)=62 and 200 GeV measured by the PHENIX detector at RHIC A.Bazilevsky Brookhaven National Laboratory.
QM2004 Version1 Measurements of the  ->     with PHENIX in Au+Au Collisions at 200 GeV at RHIC PPG016 Figures with Final Approval Charles F. Maguire.
Tomas Hreus, Pascal Vanlaer Study of Strangeness Production in Underlying Event at 7 TeV 1QCD low pT meeting, 18/03/2011.
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,
Meeting V0 Daughter PID by TPC dEdx:pp real data By AliTPCIDResponse (aleph parameterization), 4 sigma Daughter PID cuts With this K0s candidates,
Study of Charged Hadrons in Au-Au Collisions at with the PHENIX Time Expansion Chamber Dmitri Kotchetkov for the PHENIX Collaboration Department of Physics,
ATLAS ATLAS muon CSC clustering David Adams Brookhaven National Laboratory June 15, 2006 Muon Software Updated 11:00 EDT June 15, 2006.
Paolo Massarotti Kaon meeting March 2007  ±  X    X  Time measurement use neutral vertex only in order to obtain a completely independent.
Tau31 Tracking Efficiency at BaBar Ian Nugent UNIVERSITY OF VICTORIA Sept 2005 Outline Introduction  Decays Efficiency Charge Asymmetry Pt Dependence.
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.
M. Ellis - MICE Collaboration Meeting - Wednesday 27th October Sci-Fi Tracker Performance Software Status –RF background simulation –Beam simulation.
STAR Collaboration Meeting, July 16, 2002 Manuel Calderón de la Barca Sánchez StMiniMcEvent.
Software Update Takashi HACHIYA RIKEN 2012/2/10RIKEN VTX software meeting1.
Object-Oriented Track Reconstruction in the PHENIX Detector at RHIC Outline The PHENIX Detector Tracking in PHENIX Overview Algorithms Object-Oriented.
PHENIX J/  Measurements at  s = 200A GeV Wei Xie UC. RiverSide For PHENIX Collaboration.
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.
Introduction 08/11/2007 Higgs WG – Trigger meeting Ricardo Gonçalo, RHUL.
Michele Faucci Giannelli
Erik Devetak Oxford University 18/09/2008
Charles F. Maguire Vanderbilt University
Physics with the HFT prototype?
VTX tracking issues Y. Akiba.
External alignment Maya Shimomura (ISU) 12/03/15 RIKEN VTX meeting.
Lc+ Status Report Heavy Flavor Working Group
2000 Diffuse Analysis Jessica Hodges, Gary Hill, Jodi Cooley
PrimEx p0 radiative width extraction
J/Y Simulations for Trigger
Contents First section: pion and proton misidentification probabilities as Loose or Tight Muons. Measurements using Jet-triggered data (from run).
Current Status of the VTX analysis
Hit and Tracking Data set used: From loose to tight cuts Pythia p+p
Presentation transcript:

ITTF “Re-View” Session, August 11, 2003 Manuel Calderón de la Barca Sánchez ITTF Evaluation for Spectra

2 Eta Distributions

3 Eta Ratio (ITTF/TPT)

4 Pt Distribution

5 Pt Ratio (ITTF/TPT)

6 East & West vs run number

7 Looking at log For some events H No tracks are found on the east H Next event, no tracks are found on the west… H For the same event, numbers are comparable: TPTITTF Good globals H+ East H- East H+ west960 H- west870 Next event has nothing in the west… then maybe again in the east… Has to be a bug!

8 Hit and Data set used: H Hijing b<3 simulations W Usually, absolute value of efficiency is too ideal W … comparisons between current code & From loose to tight cuts H Look at midrapidity (|eta|<0.5) mainly H Accepted MC tracks == 10 MC Hits at least H Reconstructed track cuts: W Fit Points >= 10, no dca cut (3 cm for primaries) W Fit Points >= 24, dca < 1cm

9 Fit Points, Then and Now Cuts: Central Hijing Global dca<1, Fit Pts>=10 Integral normalized to 1

10 What’s the deal? Efficiency vs pT Here, efficiency is: Found & Matched MC Accepted June Review Aug. 6 Production “Loose cut” data set Tuning effort by our Wayne guys!! Note: some CVS glitch probably happened, as I’ve seen better numbers (Andrew).

11 …tighter dca and tighter fit points Cuts like those used in identified spectra papers June ReviewAug. 6 Production

12 Efficiency vs eta, tight cuts Cuts like those used in identified spectra papers Asymmetry, wasn’t there before…

13 Eta efficiency, loose cuts Zbigniew sees the same with loose cuts.

14 What’s happening?  Distribution Need to mask sectors properly

15 Efficiency and Bias Again: Current best tune was not used for this production. From Zbigniew, Bias and pulls were better before. Note scale.

16 pt Resolution

17 Curvature and tan( ) pulls.

18 Proper tuning of tracking parameters has led to improvements (Andrew). H Efficiency improved W The best tune was not used for the Hijing Masking of sectors needs to be addressed H No hardcoding of time-stamps (integration into Energy loss calculation needs to be debugged for final tuning of Must have a consistent parameter set for the production that we all use. H Need to finalize and commit BEST parameter set to the library, which gives the performance we always advertised.