Checks of TOF Fiducial Cuts

Slides:



Advertisements
Similar presentations
HARP Anselmo Cervera Villanueva University of Geneva (Switzerland) K2K Neutrino CH Meeting Neuchâtel, June 21-22, 2004.
Advertisements

1 Search for the Flavor-Changing Neutral-Current Decay,   → p     HyangKyu Park University of Michigan, Ann Arbor for the HyperCP collaboration.
Some answers to the questions/comments at the Heavy/Light presentation of March 17, Outline : 1) Addition of the id quadrant cut (slides 2-3); 2)
M. Kubantsev, ITEP/NWU BEACH-2004,ITT,Chicago, June Further (preliminary) results of re- analysis of data of the Big Bubble Chamber Neutrino.
1 G4MICE studies of PID transverse acceptance MICE video conference Rikard Sandström.
Identifying and Modeling Coronal Holes Observed by SDO/AIA, STEREO /A and B Using HMI Synchronic Frames X. P. Zhao, J. T. Hoeksema, Y. Liu, P. H. Scherrer.
1 KEK Beam Test Analysis Hideyuki Sakamoto 15 th MICE Collaboration Meeting 10 st June,2006.
Search for Thermal Photons in PHENIX - Torsten Dahms - Stony Brook University 23 rd Winter Workshop On Nuclear Dynamics February 13, 2007.
Sevil Salur for STAR Collaboration, Yale University WHAT IS A PENTAQUARK? STAR at RHIC, BNL measures charged particles via Time Projection Chamber. Due.
GlueX Particle Identification Ryan Mitchell Indiana University Detector Review, October 2004.
 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.
Background from pion beam interactions with LH2 & solid state targets J.Biernat/I.Koenig/J. Markert/W.Przygoda/P.Salabura.
Some investigations on Shower in Aug11 DST Szymon Harabasz Version: 15 November 2015.
E. De LuciaNeutral and Charged Kaon Meeting – 7 May 2007 Updates on BR(K +  π + π 0 ) E. De Lucia.
October 14, 2004 Single Spin Asymmetries 1 Single Spin Asymmetries for charged pions. Overview  One physics slide  What is measured, kinematic variables.
1 Performance of a Magnetised Scintillating Detector for a Neutrino Factory Scoping Study Meeting Rutherford Appleton Lab Tuesday 25 th April 2006 M. Ellis.
Ciro Bigongiari, Salvatore Mangano Results of the optical properties of sea water with the OB system.
1 A first look at the KEK tracker data with G4MICE Malcolm Ellis 2 nd December 2005.
Measurement of photons via conversion pairs with PHENIX at RHIC - Torsten Dahms - Stony Brook University HotQuarks 2006 – May 18, 2006.
Cedar and pre-Daikon Validation ● CC PID parameter based CC sample selections with Birch, Cedar, Carrot and pre-Daikon. ● Cedar validation for use with.
1 Nuclear modification and elliptic flow measurements for  mesons at  s NN = 200 GeV d+Au and Au+Au collisions by PHENIX Dipali Pal for the PHENIX collaboration.
 Measurement of  x E  (Fig. 4) Assorted correlations between a fixed high-p T trigger hadron (  p Ttrig  =4.7GeV/c) and lower p T associated hadrons.
Preliminary Measurement of the Ke3 Form Factor f + (t) M. Antonelli, M. Dreucci, C. Gatti Introduction: Form Factor Parametrization Fitting Function and.
Search for the  + in photoproduction experiments at CLAS APS spring meeting (Dallas) April 22, 2006 Ken Hicks (Ohio University) for the CLAS Collaboration.
T2K muon measurement 2014 Momentum module A.Ariga, C. Pistillo University of Bern S. Aoki Kobe University 1.
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 Light Yield results from the KEK tracker test using G4MICE M. Ellis Tracker Phone Meeting 25 th January 2006.
4/12/05 -Xiaojian Zhang, 1 UIUC paper review Introduction to Bc Event selection The blind analysis The final result The systematic error.
QM2004 Version1 Measurements of the  ->     with PHENIX in Au+Au Collisions at 200 GeV at RHIC PPG016 Figures with Final Approval Charles F. Maguire.
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.
Jet Production in Au+Au Collisions at STAR Alexander Schmah for the STAR Collaboration Lawrence Berkeley National Lab Hard Probes 2015 in Montreal/Canada.
CKOV1 design status 1. Generation of muon and pion beam files 2. PID performances with water radiator 3. Does it help with fluorocarbon FC72 ? 4. Conclusion.
TOF detector in PHENIX experiment PHENIX time-of-flight counter The PHENIX time-of-flight (TOF) counter serves as a particle identification device for.
Muon Trigger Performance Run12 PP510GeV Sanghwa Park (SNU/RIKEN)
2 pion photoproduction from G11A E. Golovach MSU Analysis Status for.
1 Azimuthal angle fluctuations (draft of NA49 publication) NA61/SHINE and NA49 Software/Analysis meeting February 15 th – 18 th, WUT Katarzyna Grebieszkow.
Brunel University London Field-off LiH Energy Loss Rhys Gardener CM45 – July 28th.
Comparison between Aasim and Calibob
Parameterization of EMC response for
Time Independent Analysis
Charles F. Maguire Vanderbilt University
fKK analysis in Run3 d+Au collisions: Update
Ángel Sierra, Pablo Fierro, Irais Bautista and Antonio Ortiz
NA61 and NA49 Collaboration Meeting May 14-19, 2012, Budapest
First look at data/MC comparison for period 8 reference runs
Search For Pentaquark Q+ At HERMES
Detector Configuration for Simulation (i)
Check of Lambda Simulations in TOF-West
Quarkonium production in ALICE
EMCal Recalibration Check
Run4 fK+K- analysis update
Run4 f K+K- analysis: analysis train
EMCal Recalibration Check
TOF Fiducial Cut on 325 +/- 25 MeV/c (++ Field)
EMCal Run4 Recalibration Check Looking at K mass centroid and width
J/   analysis: results for ICHEP
kT Asymmetry in Longitudinally Polarized pp Collisions
Study of e+e- pp process using initial state radiation with BaBar
->K+K- Production at 62.4GeV Au+Au Collisions
Problems with the Run4 Preliminary Phi->KK Analysis
f  K+K- analysis in Run4 Au-Au collisions at √sNN = 200 GeV
Run4 Fiducial Match between Real and MC
fK+K- yield analysis update
NKS2 Meeting with Bydzovsky NKS2 Experiment / Analysis Status
The “Other” STAR-PHENIX Discrepancy Differences in the f analyses
Low mass dimuon acceptance
Comparing Data and MC CITADL Variables on Ks and KK
Current Status of the VTX analysis
Status of the cross section analysis in e! e
Presentation transcript:

Checks of TOF Fiducial Cuts Charles Maguire Group Meeting, Nov 28

Checking Goals (TOF only here) Quantify the effect of the fiducial cuts Check all the momentum bins (showing only 0.325 MeV/c here) Look at both real data and simulation Fiducial cuts are introduced at least partially to improve the correspondence between real and simulation distributions Yield analysis should be stable if there are small changes in the fiducial cuts -- not yet confirmed by our group Current findings (using lowest momentum bin data) First quarter of ++ field runs has significant dead area (174o-178o) which was fixed in the later ++ runs and the start of the -- field runs This dead area re-appeared in second quarter of -- field runs Also a new z-localized hole in South side fourth quarter -- field runs These dead areas are not addressed so far in simulation Also determined excess fiducial cutting at lowest azimuth (< 1620) November 28, 2005 TOF Fiducial Cut Check

Z vs Phi for ++ Field First and Second Quarters (0 Z vs Phi for ++ Field First and Second Quarters (0.3 to 2 GeV/c) Dead area 174o-178o in First Quarter (not in cuts) First Quarter of ++ Field Runs Second Quarter of ++ Field Runs November 28, 2005 TOF Fiducial Cut Check

TOF Fiducial Cut on 325 +/- 25 MeV/c (++ Field) Real Data, first quarter ++ Simulation South Positive North Positive South Positive North Positive South Negative North Negative South Negative North Negative Unnecessary cutting of positive particles below 1620 (both North and South) Region 172o-178o is badly reproduced in the simulation for positive particles November 28, 2005 TOF Fiducial Cut Check

TOF Fiducial Cut on 325 +/- 25 MeV/c (++ Field) Real Data, second quarter ++ Simulation South Positive North Positive North Positive South Positive South Negative North Negative South Negative North Negative Still unnecessary cutting of positive particles below 1620 (both North and South) Region 172o-178o is better reproduced in the simulation for positive particles November 28, 2005 TOF Fiducial Cut Check

TOF Fiducial Cut on 325 +/- 25 MeV/c First Half ++ Field Sim (red line) vs Real (black points) Before Cuts Sim (red line) vs Real (black points) After Cuts South Positive North Positive South Positive North Positive South Negative North Negative South Negative North Negative Positive particle shape is not much improved using fiducial cuts Negative particle shapes were acceptable before cuts, little change after November 28, 2005 TOF Fiducial Cut Check

Third Quarter of ++ Field Runs Z vs Phi for ++ Field Third and Fourth Quarters No major differences in second half of ++ field runs Third Quarter of ++ Field Runs Fourth Quarter of ++ Field Runs November 28, 2005 TOF Fiducial Cut Check

TOF Fiducial Cut on 325 +/- 25 MeV/c Second Half ++ Field Real Data, second half ++ Simulation South Positive North Positive South Positive North Positive South Negative North Negative South Negative North Negative Positive particle shape is not much improved using fiducial cuts Negative particle shapes were acceptable before cuts, little change after November 28, 2005 TOF Fiducial Cut Check

TOF Fiducial Cut on 325 +/- 25 MeV/c Second Half ++ Field Sim (red line) vs Real (black points) Before Cuts Sim (red line) vs Real (black points) After Cuts North Positive South Positive South Positive North Positive South Negative North Negative South Negative North Negative Mostly good except for missing positive yield on North side 172o-176o November 28, 2005 TOF Fiducial Cut Check

Re-appearance of 172o-178o problems Z vs Phi for -- Field First and Second Quarters (0.3 to 2 GeV/c) Some differences between first and second quarters of -- field runs First Quarter of -- Field Runs Second Quarter of -- Field Runs Re-appearance of 172o-178o problems November 28, 2005 TOF Fiducial Cut Check

Z vs Phi for -- Field Third and Fourth Quarters (0 Z vs Phi for -- Field Third and Fourth Quarters (0.3 to 2 GeV/c) No major differences between third and fourth quarters of -- field runs Third Quarter of -- Field Runs Fourth Quarter of -- Field Runs November 28, 2005 TOF Fiducial Cut Check New small hole at z = -20 cm

TOF Fiducial Cut on 325 +/- 25 MeV/c First Half -- Field Real Data, first half -- Simulation South Positive North Positive South Positive North Positive North Negative South Negative North Negative South Negative Similar unncessary cutting below 162o in negative particles, North and South November 28, 2005 TOF Fiducial Cut Check

TOF Fiducial Cut on 325 +/- 25 MeV/c Second Half -- Field Real Data, second half -- Simulation South Positive North Positive South Positive North Positive North Negative South Negative North Negative South Negative November 28, 2005 TOF Fiducial Cut Check

TOF Fiducial Cut on 325 +/- 25 MeV/c First Half -- Field Sim (red line) vs Real (black points) Before Cuts Sim (red line) vs Real (black points) After Cuts South Positive North Positive South Positive North Positive South Negative North Negative South Negative North Negative Positive particle shape are reasonably well reproduced Negative particle shapes have the problem in the 174o-178o region November 28, 2005 TOF Fiducial Cut Check

TOF Fiducial Cut on 325 +/- 25 MeV/c Second Half -- Field Sim (red line) vs Real (black points) Before Cuts Sim (red line) vs Real (black points) After Cuts North Positive South Positive South Positive North Positive South Negative North Negative North Negative South Negative November 28, 2005 TOF Fiducial Cut Check

Explanation and Summary Slide 9 Explanation Left side is for real data and right side is for simulation: 325 +/- 25 MeV/c Real data are for all good quality tracks into TOF, first half of ++ field runs Simulation data used pions, same temperature spectrum as in real data Black line histogram is before cuts, red histogram (mostly on top of black) is for the after cuts using fiducial cut file from Dipali and Debsankar Black filled histogram is for the particles eliminated by the cuts Slide 9 Conclusion Unnecessary cutting of positive particle yield below 162 (see also slide 2) Same input as slide 1 but simulation and real results are overlaid Normalization is based on the total entries ratio (only shapes are relevant) Left side is before the fiducial cuts, right side is after the fiducial cuts Slide 9 Conclusions Also shows unnecessary cutting for positive particles below 1620 Negative particle shapes are in generally good agreement (only one big hole) Positive particle shapes above 1800 reasonably agreement between MC and Real Positive particle shapes below 1800 not as well reproduced, especially South side November 28, 2005 TOF Fiducial Cut Check

TOF Fiducial Cut on 975 +/- 25 MeV/c (++ Field) Simulation Real Data South Positive North Positive South Positive North Positive South Negative North Negative South Negative North Negative November 28, 2005 TOF Fiducial Cut Check

TOF Fiducial Cut on 975 +/- 25 MeV/c (++ Field) Sim (red line) vs Real (black points) Before Cuts Sim (red line) vs Real (black points) After Cuts South Positive North Positive South Positive North Positive North Negative North Negative South Negative South Negative November 28, 2005 TOF Fiducial Cut Check