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Update of trigger study for GMSB photons. Shilei Zang University of Colorado, Boulder. GMSB Meeting, 14th Dec. 2007. Outline. Signal efficiency Background samples processed Efficiency vs. Rates Log(eff)/log(b) vs. Cuts Preliminary results Backup slides: Eff. vs. Cuts; Rates vs. Cuts.
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Update of trigger study for GMSB photons ShileiZang University of Colorado, Boulder GMSB Meeting, 14th Dec. 2007
Outline Signal efficiency Background samples processed Efficiency vs. Rates Log(eff)/log(b) vs. Cuts Preliminary results Backup slides: Eff. vs. Cuts; Rates vs. Cuts.
GMSB sample and Background samples • Bob Hirosky’s GMSB samples at CMSSW_164 are used to estimate signal efficiency. • I used 10000 GMSB events: 900 GM1b, 800 GM1c, 1800 GM1d, 5900 GM1e, 600 GM1g. • PreCSA07 (or CSA07) samples are used to estimate the background rates, which includes: • Photon jets (all pt bin) • QCD jets (all pt bin) • Wenu, Zee, will be included in rate calculation soon. (since CSA07 Wenu sample is available just in December.)
HLT paths for photons • L1Match: Reconstructed super-cluster in the ECAL is required to match L1 energy deposit in some eta and phi windows. • Et : Et of super-cluster in the ECAL is required to exceed a threshold. • IEcal: ECAL isolation, total Et of all clusters with ΔR<0.3 around the photon candidate, excluding those belonging to the super-cluster itself. • IHcal: HCAL isolation, total Et of hadron calorimeter towers with ΔR<0.3 around the photon candidate. • Itrack: Track isolation, number of tracks with Pt>1.5GeV inside a cone ΔR<0.3 of photon candidate.
How many events in each background samples do we need to process in the rate calculation • Suppose the i-th sample has cross section σi; with a definite integrated luminosity there will be Nievents of i-th sample ; with some cuts we will select ki events; efficiency of cuts on the i-th sample is εi= ki/ Ni. • Both ki and Niare Poisson distribution, and independent, so error of εi is σ(εi)=Sqrt(εi(1+ εi)/ Ni). • With instant luminosity L, rate of i-th sample is Lσiεi, with an error of Lσiσ(εi). • To keep a small error of total rate and reduce the number of events to process, we require Lσiσ(εi)= Lσjσ(εj), so • Ni /Nj = (σi / σj)2[εi(1+ εi)]/[εj(1+ εj)]. • Process the i-th sample with small number of events (finally needs to select ~100 events, so the relative error of εi is ~10%) ; roughly determine the efficiency εiwith all default HLT paths will use. Then get the ratio of Ni /Nj.
Efficiency vs. Rates (Single Photon) • Final Rate is about : • 9.4+-0.5, for single photon path. • HLT study group resut (CMSSW131): • 8.4+-0.7.
Efficiency vs. Rates (Relaxed Single Photon) • Final Rate is about : • 3.0+-0.2, for relaxed single photon path. • HLT study group resut (CMSSW131): • 2.8+-0.2.
Efficiency vs. Rates (Double Photon) • Final Rate is about : • 0.29+-0.07, for relaxed single photon path. • HLT study group resut (CMSSW131): • 0.6+-0.4.
Efficiency vs. Rates (Relaxed Double Photon) • Final Rate is about : • 1.81+-0.15, for relaxed single photon path. • HLT study group resut (CMSSW131): • 1.8+-0.5.
Preliminary Conclusion • Rates are comparable with previous CMSSW_131 results given by HLT study group. The rates here have small errors. • From the figures, we suggest to relax the isolation cuts, especially Ecal isolation and Track isolation. We will give the suggested thresholds later. • Wenu and Zee samples will be included in rates calculation soon. Some other samples will be processed with more events.