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Isolated Prompt Photon Production in Photon-Photon Collisions at s ee =183-209 GeV T. Schörner-Sadenius on behalf of the OPAL Collaboration ICHEP 2002, Amsterdam 23-31 July 2002 ‘Prompt’ not coming from particle decays/fragmentation, but emitted from the hard underlying scattering. Abstract 376
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ICHEP02 AmsterdamSchörner-Sadenius: Prompt Photons in 2 Prompt Photons in +X Allow to study photon’s hadronic structure and test QCD predictions: Prompt appear in resolved processes (in LO; in NLO also in direct events). Small NLO corrections / scale dependency. ‘Cleaner’ than dijets (hadrons, D*) less uncertainty from hadronisation (but prompt have smaller Xsection ~O( EM )). Might further be used for studies of the underlying parton picture or background studies in LHC Higgs searches. direct resolved prompt
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ICHEP02 AmsterdamSchörner-Sadenius: Prompt Photons in 3 Theoretical Predictions Fixed-order NLO QCD calculations (Fontannaz et al). PYTHIA 6.130 for signal +X Distinct samples for single/double resolved for three energy points. Sas-1D (LO) PDF. Background with fake / real : PHOJET 1.10 and HERWIG 5.9 for background without prompt . Also Vermaseren 1.0, PYTHIA 5.7, KORALZ, grc4f. Single-resolved Double-resolved
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ICHEP02 AmsterdamSchörner-Sadenius: Prompt Photons in 4 LEP and the OPAL Detector Luminosity used: 639 pb -1
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ICHEP02 AmsterdamSchörner-Sadenius: Prompt Photons in 5 Event/ Selection ( s ee =183-209 GeV) Require 3 tracks. Reject events with scattered leptons above =33 mrad. Reject e+e- annihilations: 5 GeV < W vis < 0.3 s ee E cal < 0.25 s ee. Select isolated photons: EM clusters with | | 3 GeV. Photon and hadronic final state balanced in .
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ICHEP02 AmsterdamSchörner-Sadenius: Prompt Photons in 6 Photon Selection ctd’ Isolation criterion ( <R): Background: antineutrons, / 0 decays shape analysis: Fit: a = 0.85 0.08 (stat) b = 0.11 0.08 (stat) f max = E max /E c = ( i E i R i )/E g(f, ) = ag + bg + (1-a-b)·(cg n + (1-c)g ) i E Ti · ( -R i ) 0.2·E T (1-cos )/(1-cosR)
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ICHEP02 AmsterdamSchörner-Sadenius: Prompt Photons in 7 Single/Double Resolved Ratio r s/d For the +jet sample: using a cone jet finder with R=1, E T > 3 GeV. Fit x min distribution to data r s/d = 0.59 ± 0.12 For the complete data set use also x T =2p T /W vis r s/d = 0.41 ± 0.08, Average r s/d ~0.5. x =x = (E p z ) + (E jet p zjet ) hadrons, (E p z )
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ICHEP02 AmsterdamSchörner-Sadenius: Prompt Photons in 8 The Total Cross-Section tot = r·N prompt / single L + (1-r)·N prompt / double L N prompt : 92.8, background subtracted (FSR, , , n). r s/d :single / double resolved ratio. : Taken from PYTHIA MC (0.51 / 0.61). Tristan: (p T > 2GeV) = 1.72 0.67 pb at s ee = 58 GeV tot = 0.26 ± 0.04 (stat.) ± 0.03 (syst.) pb For isolated prompt photons (p T > 3 GeV, | | < 1):
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ICHEP02 AmsterdamSchörner-Sadenius: Prompt Photons in 9 Comparisons with PYTHIA d /dp T Shape of distributions well described, but normalisation off (1.85; in case of TOPAZ ~3, MC also low for ZEUS) d /d| |: Flat, as expected!
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ICHEP02 AmsterdamSchörner-Sadenius: Prompt Photons in 10 Comparisons with NLO Calculations Shape and normalisation correct (Fontannaz et al)! d /d| | d /dp T
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ICHEP02 AmsterdamSchörner-Sadenius: Prompt Photons in 11 Summary Prompt photons provide means to test QCD and to determine hadronic structure of photon. = 0.26 ± 0.04 (stat.) ± 0.03 (syst.) pb PYTHIA badly normalized; good agreement of differential cross-sections with NLO QCD calculations. Looking forward to final result: Test of different photon PDFs (GRV, LAC1). Investigate including FSR in signal better NLO description?
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