PrimEx p0 radiative width extraction Eric Clinton University of Massachusetts Amherst June 21, 2007 1 Outline Data Source and cuts Event selection Hybrid Mass Signal enhancement Yields Systematic effects from yield extraction Simulation Results Sytematic Error Analysis 2 Data Source and Cuts mysql -h primexdb -u primex_user book_keeping b --execute="select run from run_list where radiator='A' and target='carbon' and type='pi0' and production='good';" > run_list.example mysql -h primexdb -u primex_user book_keeping b --execute="select run from run_list where radiator='B' and target='carbon' and type='pi0' and production='good';" > run_list.example 1.) Two or more clusters/event. 2.) Minimum three (3) (PbWO4 or lead glass) detectors to define a “cluster”. 3.) 50 MeV or greater central (PbWO4 or lead glass) crystal detector energy in cluster. 4.) 10 MeV or greater minimum deposited energy in (PbWO4 or lead glass) detector. 5.) Max cluster energy 8 GeV. 6.) gg invariant mass greater than 0.085 GeV in at least one of the cluster pairs. 7.) Elasticity (cluster pair energy sum/tagger energy) greater than 0.70. 8.) Cluster energy greater than 0.5 GeV. 9.) Cluster X or Y position must be greater than 3.8 cm. 10.) Cluster pair energy sum between 3.5 and 6.5 GeV -- additional software cut not imposed on the skim, but imposed later: 11.) Timing cut of -15 ns to +5ns. “pi0gains” used as caliubration 3 Event selection Eliminate Tagger and HyCal combinatorics Likelihood Event entries have invariant mass, elasticity, and timing Fit invariant mass, elasticity, timing signal and background Fitted signal lineshape as probability density function (PDF) Which entry to choose in a mutli-entry event? Which is "most likely"? Evaluate the PDF for each parameter for each entry. Three individual likelihoods. PDFInvariant mass, PDFElasticity, PDFTiming Total likelihood = PDFInvariant mass × PDFElasticity ×PDFTiming Entry with highest total likelihood "wins". 4 Getting Final Likelihood spectrum Take entire “Most Likely” spectrum as event sample Most Likely invariant mass spectrum Final Likelihood PDFInvariant mass × PDFElasticity ×PDFTiming 5 Misidentification – any systematics? No. MisID is random, and event selection tends to pick smaller production angle pions. 6 Rotation of 2-D data onto 1-D Try to enhance signal to noise Original 2-D data Elasticity vs.Invariant Mass New 1-D signal AKA “Hybrid Mass” 7 Selected Hybrid Mass Fits 8 p0 yields as a function of production angle. 9 Systematic error sources? Extracted yields over the entire pion angle range must be stable as these parameters are varied. 10 Lineshape Degrees of Freedom entire HyCal acceptance 11 Integration/BG subtraction range entire HyCal acceptance 12 Stability of Fit Range entire HyCal acceptance 13 The Veto—how it changes the angular spectrums 14 Extracting a Photon Misidentification Efficiency PME = 0.76% 15 Simulation Work Thrown with E-Channel Photon flux weighting Energy correction added Proper shower development Resolution and centroid tuned Energy lost out back of HyCal, out of cluster mask Added back about 10% of energy Tracking threshold tuned Primakoff (with FSI), Coherent (Cornell with FSI), Incoherent (Glauber) Get invariant mass right to proper mock physics Vet the Simulation Push 4 vectors from experiment thru sim See how p0 candidate spectrum look, look for losses Turn off detectors, see how acceptance behaves 16 Photon flux 17 Poor Elasticity 18 Energy Correction Across entire HyCal acceptance 19 Tracking Threshold, resolution, and centroid tuning 20 Putting physics events thru the Simulation Around 99.2% fidelity 21 Turning off glass detectors Entire HyCal Acceptance 22 Turning off tungstate detectors Entire HyCal Acceptance 23 Turning off glass detectors HyCal Tungstate Acceptance Only 24 Efficiencies as a function of the photo-pion process, entire HyCal acceptance 25 Geometric efficiency and reconstruction (cut) efficiency. Entire HyCal Acceptance 26 Efficiencies as a function of the photo-pion process, HyCal Tungstate acceptance 27 Geometric efficiency and reconstruction (cut) efficiency HyCal tungstate acceptance 28 Fit to Data, and Extracted Width Entire HyCal Acceptance Extracted width – 7.870 eV ± 0.139 eV (1.77%) 29 Fit to Data, and Extracted Width HyCal Tungstate Acceptance Extracted width – 7.859 eV ± 0.146 eV (1.86%) 30 Acceptance Corrected Cross Sections Entire HyCal Acceptance HyCal Tungstate Acceptance 31 Systematic Error Entire HyCal acceptance Nominal 7.870 NA Fit Range (nominal = ±0.030 HMU’s Veto width: 7.779 -1.16 Cluster Position Finding Method 7.720 7.888 7.938 7.849 -1.90 0.23 0.86 -0.27 Lineshape (degrees of freedom)*** Method 0: Method 1: Method 2: Method 4: DG3Sp: TG3Po: 7.859 7.931 -0.14 0.77 * (+) * (-) * (+) 3% width: 2% width: 0.5% width: 0.3% width: 0.2% width: 7.802 7.841 7.966 7.966 8.001 -0.86 -0.36 1.22 1.22 1.67 * (-) 7.760 7.973 -1.40 % 1.31 % -30, +33 -30, +27 7.838 7.877 -0.41 % 0.09 % -27,+30 -33, +30 7.745 8.002 -1.58 % 1.68 % Average = Average = Average 7.867 7.862 7.870 -0.03 % *(-) -0.10 % *(-) 0.04 % (+) Adding the *(+) gives positive sytematic shift +1.46 Adding the *(-) gives negative systematic shift -0.88 Systematic Error = +1.46, -0.88 Integration range (Nominal cutoff = 1.0%) -27, +27 -33, +33 *(+) ***Nominal = Double gaussians with 3rd order polynominal DG3Sp = Double gaussians with 3rd order spline TG3Po = Triple gaussians with 3rd order polynominal 32 Systematic Error HyCal Tungstate acceptance Nominal 7.859 NA Fit Range (nominal = ±0.030 HMU’s Veto width: 7.774 -1.16 Cluster Position Finding Method 7.699 7.827 7.881 7.670 -2.04 -0.41 0.24 -2.40 Lineshape (degrees of freedom)*** Method 0: Method 1: Method 2: Method 4: DG3Sp: TG3Po: 7.859 7.891 -0.00 0.41 * (-) * (-) * (+) 5% width: 2% width: 0.5% width: 0.2% width: 0.1% width: 7.788 7.813 7.877 7.938 7.926 -0.90 -0.59 0.22 1.00 1.31 7.809 7.888 -0.63 % 0.36 % -30, +33 -30, +27 7.824 7.888 -0.45 % 0.36 % -27,+30 -33, +30 7.777 7.941 -1.04 % 1.04 % Average = Average = Average 7.867 7.862 7.870 -0.1 % *(-) -0.03 % *(-) 0.00 % (+) Adding the *(+) gives positive sytematic shift +1.08 Adding the *(-) gives negative systematic shift -0.99 Systematic Error = +1.08, -0.99 Integration range (Nominal cutoff = 1.0%) -27, +27 -33, +33 * (-) *(+) ***Nominal = Double gaussians with 3rd order polynominal DG3Sp = Double gaussians with 3rd order spline TG3Po = Triple gaussians with 3rd order polynominal 33 Total Error budget Entire HyCal Acceptance HyCal Tungstate Acceptance Statistical Statistical Veto Off ± 1.77 Veto Off ± 1.86 Veto On ± 1.62 Veto On ± 1.75 Photon Flux Systematic (Yield Extrn.) Branching Ratio Target Thickness Veto (if used) ±1.10 Photon Flux +1.46, -0.88 Systematic (Yield Extrn.) Branching Ratio ±0.03 Target Thickness ±0.04 Veto (if used) ± 0.05 ± 0.03 ± 0.04 ± 0.05 ±1.10 +1.08, -0.99 34 Result Entire HyCal Acceptance Gp0 = 7.870 eV ± 0.139 eV +0.144 eV – 0.111 eV Gp0 = 7.870 eV ± 1.77 % +1.83% - 1.41% HyCal Tungstate Acceptance Gp0 = 7.859 eV ± 0.146 eV +0.121 eV – 0.116 eV Gp0 = 7.859 eV ± 1.86 % +1.54% - 1.48% 35 Future work Work another nuclear incoherent generator Evolve cross sections to the weighted mean photon energy Lead Target Data? 36
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