Muon PRS Report Tasks & Manpower Needs DC04 Preparations High Momentum Muon Reconstruction H → 4µ Studies Darin Acosta PRS Task List and Manpower As part of the CPT Annual Review and the LHCC review, we were asked to provide a task list for the next couple years and the estimated manpower required Tasks: Î Simulation Î Reconstruction Î Calibration & Alignment Î Data Handling & Monitoring Î L1 Trigger Simulation Î HLT Î Testbeam Software EMU Meeting, 19 Oct 2003 2 Annual Review Recommendations Recommendations (in Order of Priority): 1. A renewed effort is needed in detector calibration. This includes all the PRS detector groups as well as calibration infrastructure from CCS. Since an exercise of calibration was already planned for DC04 as input to the computing TDR, this is clearly an urgent problem. 2. The detector groups should supply manpower to perform time critical activities such as calibration. 3. PRS should participate in the specification of a minimal (Distributed) Analysis Model which can be implemented in time for the Physics TDR. In fact, it would be good if we could have an implementation to study in time for the Computing TDR. 4. PRS should rapidly move to produce persistent physics objects in the new framework. EMU Meeting, 19 Oct 2003 3 PRS Tasks & Estimated Manpower Needs Muons (FTE) Simulation 2003 2003 (now) (need) 1.5 (Geometry, simHits, digitization, Validation, CommonDet and Tracker domains, fast simulation) 8 Reconstruction 2 (pulse reconstruction; maintenance and development of clustering algorithms) 5 Calibration (Simulation studies, application of constants) Data handling & Monitoring 0.5 2004 2005 2006 2007 2.5 2.5 2.5 2.5 2.5 2.5 4 4 3 4 2 4 4 4 4 0.5 2 3 2 3 2 0.3 (Any off-line and quasi-online software needed to cope with real data, Tracker and DAQ Proto.) 0 Level-1 Trigger simulation 2 2 1.5 1 1 2 HLT 1 1.5 4 4 3 5 4 4 4 4 4 15 22 22.5 19.5 24.5 muon object reconstruction, and full analysis like for Physics TDR 10 Test-beam software and analysis 4 (Normally included in Data handling and Monitoring) 12 TOTAL EMU Meeting, 19 Oct 2003 11.3 4 Effort needs to double in the next year Simulation Tasks √ Final adjustments & tuning to OSCAR (Geant-4 detector simulation) √ Refinement of simulation based on testbeam results Implementation of muon performance parameterizations into FAMOS (fast detector simulation) Development of a long-term supportable XML geometry description for DDD (and short term maintenance/update of existing XML) √ Support for the production of necessary MC samples for muon analyses ( √ = task started, partially covered) EMU Meeting, 19 Oct 2003 5 Reconstruction Tasks √ Further improve/optimize local reconstruction (DT, CSC, RPC) Î In presence of backgrounds Î From results of testbeam studies Î Develop tools for MC/testbeam comparison √ Optimize global reconstruction for efficiency, speed, rate reduction: Î Define/implement “reconstruction geometry” (different level of details than “simulation geom.”; same DDD source ) Î Develop improved navigation & extrapolation tools Î Develop improved B-field tools (data retrieval, interpolation) EMU Meeting, 19 Oct 2003 6 Calibration & Alignment Tasks For DT, CSC, RPC separately: Î Establish calibration procedures, frequency, and data volume Î Define format of constants stored in DB Î Possibly transfer exisiting data from chamber/electronics production DB to CMS-wide DB (once latter is defined) Î Define interface between DB and HLT/reconstruction code Î Develop software to apply DB constants to HLT/reconstruction Same for alignment (⇒ constants from alignment hardware) Additionally: √ Î Interface “misalignment tools” to “reconstruction geometry” √ (from DDD) in ORCA Î Develop calibration strategies & software (e.g. vs magnetic field knowledge) Î Develop alignment strategies with tracks & software (“internal” barrel/endcap, overlap region, muon-Tracker ) EMU Meeting, 19 Oct 2003 7 Data Handling & Monitoring Tasks Define monitored quantities and possible alarms for DCS Define monitored quantities and tolerance criteria for online farm Î Probably a lot of experience at FAST sites… Develop software to produce histograms and alarms from online data, HLT monitoring (once CMS-wide framework developed) Define muon data sets (streams) and data volume √ Î Single muon and di-muon streams Î Other physics streams? Î Prescaled loose triggers (e.g. HLT pass-through triggers) Define data handling procedure for reconstruction (application of calibration and alignment corrections) √ Introduce realistic data formats in HLT processing in ORCA Î Started in “slice test” software development EMU Meeting, 19 Oct 2003 8 L1 Trigger Simulation Tasks Update L1 simulation to exactly match electronics algorithms: √ Î RPC trigger with 4/6 logic and HO added √ Î DT BTI+TRACO+TSS updates Î RPC → CSC interface (TMB) Refine L1 algorithms to further improve efficiency, rate reduction and functionality: √ Î CSC single µ trigger for |η|>1.6 without RPC and ME4/2 √ Î CSC di-muon trigger with increased η coverage (See Alexei’s talk) Î Cosmic ray trigger We’ll need a cosmic trigger for slice tests on the surface Î Accelerator muon trigger Needed for beam running (alignment studies) EMU Meeting, 19 Oct 2003 9 HLT and Full Analyses √ Minimize HLT execution time Adapt HLT code to any specific online filter farm requirements √ Refine HLT algorithms to further improve efficiency, rate reduction and functionality (especially based on analyses) Muon reconstruction at very high pT Î Study/optimize performance √ Muon identification Î Isolated & inside jets (⇒ b-physics) √ Perform full analysis of H → 4µ Î No U.S. group? √ Perform full analysis of H → 2µ √ Perform full analysis of Z' → 2µ EMU Meeting, 19 Oct 2003 10 For Physics TDR Test Beam Software & Analysis √ Integrate testbeam DAQ software into ORCA framework Log data into native ORCA data format Work of R.Wilkinson for EMU, with P.Kreuzer (UCLA) joining Î Develop testbeam geometries (prototype exists for Barrel with simple “one-station” setup) M.Case (UCD) assists for EMU (?) Î √ Perform analysis of local reconstruction quantities (e.g. residuals) for comparison and tuning of detector simulation Î Could benefit from an analysis of the latest CSC beam test data with production electronics Perform dedicated mini-experiments (e.g. scattering in iron) to check HLT and validate Geant4 physics simulation Î Develop software for 2 stations setup (geometry, L1 TrackFinder LUTs, reconstruction...) testbeam software into system software for slice tests of √ Evolve many chambers and for CMS commissioning Î Starting for CSCs EMU Meeting, 19 Oct 2003 11 DC04 Status The 2004 Data Challenge is a 50M event production Î In fact 70M Pythia events were requested by the PRS groups Î 35M events have already been pushed through CMSIM OSCAR (G4) is ready for detector simulation Î Will be used for all PRS/µ samples except W/Z (i.e. we’ve been waiting…) ORCA is about ready for digitization Î First 4M events will be ready within a month 0.7M requested by PRS/µ: single muons, high-mass DY, t-tbar events Î Remaining 46M available after Feb’04 challenge Data will be available at CERN or FNAL Î But perhaps not at both EMU Meeting, 19 Oct 2003 12 High Momentum Muon Reconstruction Improvement to muon reconstruction algorithm driven by physics study of Z’ search Î Work of R. Cousins and J. Mumford (UCLA) Î Significant tails in mass resolution of high-mass di-muon pairs are a major source of background for the Z´ signal Î Would like to reduce tails while maintaining or improving Z´ FWHM Detailed report given at Muon PRS Meeting during Sept’03 CMS Week EMU Meeting, 19 Oct 2003 13 Some Possible Track Fitting Methods GMR • • 5 Parameter measurement at inner surface of tracker from backward part of Kalman filter fit to tracker and muon hits (default L3 fitting method). http://agenda.cern.ch/askArchive.php?base=agenda&categ=a03423&id=a03423s1t0/transparencies for more information. Tracker System Tracker Only • • Measure here Use scaled final forward values to initialize backward filter Muon System Forward filter Backward filter Iron CSC, DT Use only tracker hits for Kalman filter. Take measurement from innermost tracker surface. Available as reconstruction option in ORCA 6.3.0 (implementation by Norbert Neumeister). Tracker System Muon System Tracker + 1 Muon-Station • Use tracker and hits from first muon station which contains hits. Tracker System µ-PRS Meeting: September 16 , 2003 Muon System R. Cousins, J. Mumford UCLA 4 1/pT Resolution : Fit Comparison I Entries GMR eta < 1.04 Entries 160 140 "Barrel" 0.01098 RMS 0.1577 Underflow 120 In barrel, tracker-only has smaller tails, (truncated) RMS 1068 Mean 0 Overflow 18 100 Tracker Only Entries 80 60 eta < 1.04 Entries 160 1068 Mean 0.0005788 RMS 140 40 120 0.1184 Underflow 0 Overflow 6 20 Tracker + 1 mu-station -0.8 -0.6 -0.4 -0.2 -0 0.2 0.4 0.6 0.8 1 ((1/pT)rec - (1/pT)gen)/(1/pT)gen Entries 80 60 GMR Entries Mean "Endcap" RMS 120 40 670 -0.009759 0 20 Overflow 7 0 -1 160 Mean 1068 0.005602 RMS 120 0.133 Underflow 0 Overflow 13 100 0.1689 Underflow eta < 1.04 Entries 140 eta > 1.04 160 140 Entries 100 0 -1 -0.8 -0.6 -0.4 -0.2 -0 80 0.2 0.4 0.6 0.8 1 ((1/pT)rec - (1/pT)gen)/(1/pT)gen 60 100 Tracker Only Entries 80 60 eta > 1.04 Entries 160 40 120 20 -0.01675 RMS 140 40 670 Mean 0.1849 Underflow 0 Overflow 5 0 -1 -0.8 -0.6 -0.4 -0.2 -0 0.2 0.4 0.6 0.8 1 ((1/pT)rec - (1/pT)gen)/(1/pT)gen 20 Tracker + 1 mu-station -0.8 -0.6 -0.4 -0.2 -0 0.2 0.4 0.6 0.8 1 ((1/pT)rec - (1/pT)gen)/(1/pT)gen Entries 100 0 -1 80 60 RMS 120 20 ORCA 6.3.0 Digis ORCA 6.3.0 MuonAnalysis package Drell Yan Mass > 1.5 TeV Sample pT > 100 GeV Mean 140 40 0 -1 eta > 1.04 Entries 160 671 -0.01558 0.1467 Underflow 0 Overflow 4 100 -0.8 -0.6 -0.4 -0.2 -0 0.2 0.4 0.6 0.8 1 ((1/pT)rec - (1/pT)gen)/(1/pT)gen 80 60 Differences between fits in endcap less clear µ-PRS Meeting: September 16 , 2003 40 20 0 -1 -0.8 -0.6 -0.4 -0.2 R. Cousins, J. Mumford UCLA -0 0.2 0.4 0.6 0.8 1 ((1/pT)rec - (1/pT)gen)/(1/pT)gen 5 1/pT Resolution : Fit Comparison II eta < 1.04 50 40 30 1068 0.0007453 0.08179 23 58 108.7 / 86 0.0494 33.86 ± 1.62 0.002935 ± 0.00211 0.06216 ± 0.00213 In barrel and endcap, tracker + 1 mu-station has best fitted-sigma 0.062 Tracker Only 20 50 10 40 30 -0.2 -0.1 0 1068 -0.0005495 0.09854 12 18 105.2 / 89 0.1153 24.76 ± 1.107 -0.0003817 ± 0.003048 0.09069 ± 0.002867 0.1 0.2 0.3 ((1/pT)rec - (1/pT)gen)/(1/pT)gen 20 eta > 1.04 Entries Mean RMS Underflow Overflow χ2 / ndf Prob Constant Mean Sigma 60 50 40 30 670 -0.000949 0.09816 26 26 98.92 / 82 0.09837 16.79 ± 1.171 -0.002843 ± 0.00338 0.07455 ± 0.004219 0.075 20 0 -0.3 -0.2 -0.1 0 0.1 0.2 0.3 ((1/pT)rec - (1/pT)gen)/(1/pT)gen eta < 1.04 Entries Mean RMS Underflow Overflow χ2 / ndf Prob Constant Mean Sigma 60 50 40 0 -0.3 -0.2 -0.1 0 0.1 0.2 0.3 ((1/pT)rec - (1/pT)gen)/(1/pT)gen Tracker Only 30 eta > 1.04 Entries Mean RMS Underflow Overflow χ2 / ndf Prob Constant Mean Sigma 60 50 40 10 Tracker + 1 mu-station 10 Entries Entries GMR 0.091 Entries 0 -0.3 eta < 1.04 Entries Mean RMS Underflow Overflow χ2 / ndf Prob Constant Mean Sigma 60 30 670 -0.00588 0.1041 36 27 90.03 / 88 0.42 12.97 ± 0.879 -0.007093 ± 0.004398 0.09662 ± 0.005328 0.097 20 0 -0.3 -0.2 -0.1 0 -0.1 0 0.1 0.2 0.3 ((1/pT)rec - (1/pT)gen)/(1/pT)gen ORCA 6.3.0 Digis ORCA 6.3.0 MuonAnalysis package Drell Yan Mass > 1.5 TeV Sample pT > 100 GeV 0.1 0.2 0.3 ((1/pT)rec - (1/pT)gen)/(1/pT)gen Tracker + 1 mu-station eta > 1.04 Entries Mean RMS Underflow Overflow χ2 / ndf Prob Constant Mean Sigma 60 50 40 -0.2 30 671 -0.001058 0.08231 24 11 83.81 / 75 0.2275 19.49 ± 1.213 -0.000199 ± 0.002979 0.06841 ± 0.003234 0.068 20 10 0 -0.3 µ-PRS Meeting: September 16 , 2003 0.051 10 10 0 -0.3 1068 0.004161 0.07089 20 36 115.7 / 75 0.001778 42.53 ± 1.869 0.005539 ± 0.00174 0.05062 ± 0.001485 20 Entries Entries Mean RMS Underflow Overflow χ2 / ndf Prob Constant Mean Sigma 60 Entries Entries GMR -0.2 -0.1 R. Cousins, J. Mumford UCLA 0 0.1 0.2 0.3 ((1/pT)rec - (1/pT)gen)/(1/pT)gen 6 A Prototype Selection Criterion Using “Prob” in Tail of F2 Distribution > Observed F2 4. If difference is greater than 50 (optimized value), replace with tracker-only fit. Track is now referred to as “optimized”. Replace with tracker-only 160 140 30 -ln(Prob) of replacement muon from tracker-only. 25 120 20 Entries 119 Mean 3.676 RMS 7.749 Underflow 0 Overflow 0 100 15 80 60 ~11% of tracks in "barrel" 10 40 0 0 5 No change 20 5 10 15 20 25 30 35 eta > 1.04 Entries 671 Mean x 2.227 Mean y 3.39 RMS x 5.07 RMS y 6.618 44 7 0 0 620 0 0 0 0 200 180 Replace with tracker-only 160 140 0 0 40 45 50 -ln(Prob) Tracker 10 15 20 25 30 35 40 45 50 -ln(Prob) Replacement Entries 44 Mean 3.657 RMS 8.02 Underflow 0 Overflow 0 18 16 14 12 100 10 80 8 60 6 ~7% of tracks in "endcap" 4 No change 20 0 0 5 eta > 1.04 120 40 ORCA 6.3.0 Digis ORCA 6.3.0 MuonAnalysis package Drell Yan Mass > 1.5 TeV Sample Muon pT > 100 GeV eta < 1.04 Events 180 1068 2.512 4.423 4.419 7.05 2 0 0 Events 3. Check difference in -ln(Prob) between tracker + 1 mustation and trackeronly fits eta < 1.04 Entries Mean x Mean y RMS x RMS y 0 119 0 947 0 0 200 -ln(Prob) Tracker + Mu-Station 2. Start with tracker + 1 mu-station fit. -ln(Prob) Tracker + Mu-Station 1. 5 10 15 20 25 30 35 40 45 50 -ln(Prob) Tracker µ-PRS Meeting: September 16 , 2003 2 0 0 5 10 15 20 25 R. Cousins, J. Mumford UCLA 30 35 40 45 50 -ln(Prob) Replacement 11 Zssm (3 TeV) vs Drell-Yan background Optimized Opp-sign dimuon mass 45 Events/100 GeV/100 fb-1 Events/100 GeV/100 fb-1 Default GMR Opp-sign dimuon mass 40 35 30 45 40 35 30 25 25 20 20 15 15 10 10 5 5 0 1500 2000 2500 3000 3500 ORCA 6.3.0 Digis MuonAnalysis package Note: Optimization algorithm was tuned on different sample. 4000 4500 5000 mu+ mu- mass 0 1500 2000 2500 3000 3500 4000 4500 5000 mu+ mu- mass Optimized has narrower signal, perhaps reduced background tails. µ-PRS Meeting: September 16 , 2003 R. Cousins, J. Mumford UCLA 15 H→4µ Full Analyses Two groups have started investigations using CMSIM & ORCA Î Karlsruhe Concentrating on low mass region MH < 2MZ mostly Î INFN Firenze Concentrating on high mass region MH > 2MZ mostly CMS-IN 2003-046 Work is under review by PRS Higgs and Muon groups Î Only results approved during a PRS plenary meeting can be released publicly for conferences (Nov. CPT Week in this case) EMU Meeting, 19 Oct 2003 14 Preselection Signal and background after preselection (L = 20 fb-1): Selection optimized for MH > 2MZ and MH < 2MZ . Matteo Sani - PRS mu, 14/10/2003 7 Selection (MH > 2MZ) di-muon mass: both muon pairs with an invariant mass mµ + µ − − M Z < 8.0 GeV/c2 transverse momenta – thresholds at 20, 15, 15, 10 GeV/c pT of the Higgs candidate Matteo Sani - PRS mu, 14/10/2003 8 Efficiencies (MH > 2MZ) reco Z mass + pT pT4µ tt 42.4 % 0.05 % 0.05 % Zbb 40.2 % 0.3 % 0.3 % ZZ 68.6 % 35.8 % 15.2 % H (200 GeV/c2) 71.4 % 49.4 % 37.4 % H (300 GeV/c2) 76.7 % 51.5 % 42.1 % H (500 GeV/c2) 76.6 % 50.6 % 43.8 % Signal and background after the selection described before (L = 20 fb-1) Matteo Sani - PRS mu, 14/10/2003 10 1 fb ) Results (L = 20 (MH < 2MZ) (MH > 2MZ) |mµµ- MZ|< 6 GeV/c2 |mµµ- MZ|< 8 GeV/c2 pT thres. (20, 15, 10 , 7 GeV/c) pT thres. (20, 15, 15, 10 GeV/c) iso.: ∆R=0.2, pTmax = 4.0 GeV/c four µ system pT > 15 GeV/c -0.9 < cosθD < 0.8 MH (GeV/c2) Higgs ZZ(*) tt Zbb 130 5.0 0.65 < 0.5 1.2 150 10.9 0.71 < 0.5 < 1.7 200 19.4 2.5 0.35 < 1.7 300 13.9 2.0 < 0.5 < 1.7 500 7.0 1.5 < 0.5 < 1.7 Matteo Sani - PRS mu, 14/10/2003 Events falling inside ±2σH When no events are found the upper limit at 68 % C.L. is given 16 after all cuts (20 fb-1) after isolation cut with default value after all cuts (20 fb-1) after optimized isolation cut isolation cut improves signal visibility significantly Valeria Bartsch, CPT week, May 2003 9 mH [GeV] Valeria Bartsch, CPT week, May 2003 12 Conclusions With CSC production nearly over, FAST sites nearly finished, and installation well in hand: Î Need to transfer experience to PRS groups! Especially in the areas of local reconstruction, test beam analysis, calibration & alignment schemes, data handling & monitoring Physics studies are starting to drive reconstruction improvements Î Muon reconstruction in Z’ search Î Isolation techniques for H→4µ studies EMU Meeting, 19 Oct 2003 15 Recent Agenda EMU Meeting, 19 Oct 2003 16