hlt met noise filters in run2011b
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HLT MET Noise Filters in Run2011B Alex Mott Caltech Review of - PowerPoint PPT Presentation

HLT MET Noise Filters in Run2011B Alex Mott Caltech Review of Noise Filters HBHE noise filters were deployed online earlier this year Based on the offline Hcal HBHE Noise filters used in the PromptReco For HLT, add an additional


  1. HLT MET Noise Filters in Run2011B Alex Mott Caltech

  2. Review of Noise Filters ● HBHE noise filters were deployed online earlier this year ● Based on the offline Hcal HBHE Noise filters used in the PromptReco ● For HLT, add an additional safety factor to avoid rejecting possible good physics events ● If there are two or more additional RBXs with energy > 40 GeV, do not reject the event ● This filter was shown to overclean at HLT less then 1 ppm ● We intended to deploy this filter as part of the default HLT MET this fall ● Move to beta*=1m delayed this ● Performance of the filters degraded in Run 2011B – needed time to study

  3. Scaling with Luminosity Run2011A Run2011B High PU Fill – ZeroBiasHPF0 PD Fraction of Events Rejected MET PD Offline Filter Online Filter ● The online HBHE Noise Filter is becoming considerably less efficient in rejecting noise as pileup increases ● The offline filter seems to be much less sensitive to the increase in pileup

  4. Online Filter Inefficiency Frac of Events Passing 3 rd RBX Cut High PU Fill ZeroBiasHPF0 Fraction of events 40 50 60 With 3 rd RBX GeV GeV GeV E>40 GeV CaloMET > 60 GeV ● One issue is with the online safety cut ● At higher pileup, even Zero Bias events pass the cuts a substantial fraction of the time ● Raising the cut is dangerous ● The pileup falls off substantially over the course of the run ● Even at peak PU, there is a fairly large range of pileup possible event-by-event

  5. Modifying the Online Filter ● The 40 GeV threshold is too low for the expected peak 2012 pileup conditions ● Simple raising the threshold is suboptimal for long fills with large pileup decay ● Two better options for modifying the limit: ● Inst. Lumi dependent: set the energy threshold as a function of the luminosity (need to check if this is technically possible) ● Event-by-Event: do something like L1FastJet to subtract the pileup energy on an event by event basis – keep 40 GeV threshold ● Perhaps we should consider adding a second, higher mass cut and accepting events passing this regardless of the noise filter ● i.e. for the HLT_MET200 path, only check the online noise filter for MET between 200 and 300 GeV ● This would suppress the trigger rate while still keeping full efficiency for very high MET events

  6. Reducing the PU Effect One Idea: Apply an energy correction Frac of events passing online ● safety cut analogous to L1FastJet High PU Fill Order the RBXs by energy ● ZeroBiasHPF0 Compute the median energy of all RBXs > ● 5GeV except the 3 highest energy Subtract this from the energy of the ● third highest energy RBX, treat this as the energy for the purpose of the safety cut Run177201 Run177201 ZeroBias Energy Subtracted ZeroBias By this algorithm Energy of 3 rd RBX

  7. Performance on High MET Events ● On very high MET events, the reduction isn't as dramatic as on ZeroBias This is not fully understood ● Would expect most of these events to ● be RBX noise overlaid on Zero Bias Run 177201 If this effect is real, need to ● MET PD understand why HLT_MET200 skim Perhaps there is other pathology ● in high MET events ● Its possible that these events are more empty than normal zero bias ● Would need to tune the subtraction algorithm ● Would accomplish a 50% reduction on the HLT_MET200_HBHENoiseFiltered path at the current pileup ● This is just a first test ● Suggestions for subtraction algorithm welcome

  8. Removing the Noise from MET ● Try to estimate the MET the event would have had if not for the HBHE Noise ● Correct the MET in two possible ways ● Set the energy in all hits in the noisy RBX to 0 ● Treat the noisy energy as having energy equal to the second highest energy RBX ● Choose the larger of these two values as the “corrected MET” ● Try to define this in the safest way possible to always over estimate the corrected MET ● Apply a looser threshold to this corrected MET

  9. Corrected MET Trigger Accept the event is cMET is greater than half the HLT MET threshold ● Half is just an initial test –> can be tuned ● Could conceivably try to recover events with MET lost by opposing HBHE ● Noise This is a very rare case, and may not be worth the effort ● This method could, in principle, reject a hard interaction coincident with ● HBHE Noise This event either had little real MET, so shouldn't have passed a MET ● trigger anyway Or had unbalanced energy coincident with the noise → probably ● unrecoverable offline anyway Accept Event NO YES YES MET MET MET MET HBHE Remove Recompute RECO RECO > 100 GeV? > 200 GeV? Noise? Noise MET NO NO Reject Event

  10. Effect of the MET Cleaning Run 177201 MET PD HLT_MET200 Skim Events rejected by offline noise filter 80% reduction in MET200 Trigger Rate

  11. Conclusion ● The noise cleaning efficiency of the online filters has decreased in Run2011B This is an inevitable consequence of the increased pileup ● ● Simply raising the threshold of the RBX safety cut is one possibility ● This doesn't take into account the change in PU conditions during the fill ● First attempt at introducing some pileup scaling in the cut shows modest gains in noise rejection efficiency – Retune the scaling to maximize rejection – Safety for signal still needs to be evaluated ● An alternative to doing the scaling is to try to estimate the MET without the spike and cut on that ● This shows the potential to greatly reduce rates ● Needs careful study for signal safety!!

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