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Using direct photons to calibrate/monitor L1Calo. Hardeep Bansil University of Birmingham L1Calo Joint Meeting, Heidelberg January 11 – 13, 2010. Talk Outline. Direct Photons Motivation Analysis Results so far Next steps Data so far Summary. Direct Photons. - PowerPoint PPT Presentation
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Using direct photons to calibrate/monitor L1Calo
Hardeep BansilUniversity of Birmingham
L1Calo Joint Meeting, HeidelbergJanuary 11 – 13, 2010
Talk Outline
• Direct Photons• Motivation• Analysis• Results so far• Next steps• Data so far• Summary
2
Direct Photons
• ‘Direct’ or ‘prompt’ photons originating directly from hard pp interaction
• Leading order processes – Compton (qg)
– Annihilation (qq)
3
Francesca Bucci, 10/2008, Direct Photons at ATLAS
Direct Photons• Have a γj final state• Background from
‘fake’ photons created in the jet
• Long term strategy – Select events that were triggered by jet and get efficiency for γ (and vice versa)
4
Direct photon event signature seen in ATLANTIS Event Display, Mark Stockton, Production of Direct Photons at ATLAS, 6-8/4/2009
Direct Photons• Jet and photon in event• Higher cross section than Z→ee (approx 2
orders of magnitude)
• γ complementary to e but still isolated5
Carminati, 28/8/2009
Motivation
• Using direct photons for:– Efficiency determination of electromagnetic and
jet triggers– Monitoring and calibration of L1Calo with physics
objects
6
Analysis
• Using Athena version 15.5.1• Using Analysis package from John Morris
– with some modifications!
• Using MC Direct Photon data files– PYTHIA, √s = 10 TeV, pT > 150 GeV
• Get reconstructed offline photons in each event• Select the photon with highest ET
• Compare with EmTau RoIs
7
Results so far• Distributions for highest ET offline reconstructed photons
• MC pT cut at 150 GeV – v. high
• Want to look at lower energies
8
Results so far
• Resolution in η, Δη = ηOfflinePhoton – ηEmTauRoI
10
All Photons Direct Photons (> 50 GeV)
Results so far
• Resolution in φ, Δφ = φOfflinePhoton – φEmTauRoI
11
All Photons Direct Photons (> 50 GeV)
Results so far• Calculate Δr = √((Δη)2+(Δφ)2) using offline photon and
EmTau RoI• Good photons have Δr < 0.4, ignore the rest (less than
5%)
12
Results so far• Look at ‘triggered’ EmTau RoIs again (Δr < 0.4)• ET distribution matches offline highest ET
photon better
13
• EmTau RoI v Offline Photon Energy– EmTau RoI energies seem higher than those for photons
Results so far
14
Fake photons
Direct photons
Results so far• Resolution in ET = (ET,Phot- ET,RoI)/ET,Phot
15
All Photons Direct Photons (> 50 GeV)
Results so far• Trigger Isolation Energy – observe ET behaviour when
isolation is / is not set for EmTau RoI thresholds• All γ
• Highest ET γ
Bit 01 – No Isolation, ET > 7 GeV Bit 05 – Isolation < 5 GeV, ET > 20 GeV
16
Results so far• Efficiency in ET for EmTau RoIs =
RoI Δr < 0.4 & EM/TAU Threshold passedRoI Δr < 0.4
17
Bit 06 – Isolation < 5 GeV, ET > 24 GeVBit 02 – No Isolation, ET > 14 GeV
Big loss at low ET
Results so far• Efficiency in ET – this time for offline photons
• Not as clean as for RoIs18
Bit 02 – No Isolation, ET > 14 GeV Bit 06 – Isolation < 5 GeV, ET > 24 GeV
Next steps
• Check code with other simulated direct photon datasets– Direct photons generated with lower ET threshold
• Comparisons of reconstructed offline photons with truth level
• Looking at real data!
19
Data so far• Run 142193, 900 GeV, 152000 events in
dataset) – 101 medium offline electrons found• Still too low statistics to do proper analysis
20
Juergen Thomas, 20/12/2009
Summary• Direct photons• Monitor / calibrate• Good results with current MC data• Look at more data
21