1 / 37

Data Taking Efficiencies

CDF Performance and Improvements Detectors, Triggers, Offline, and Analysis Algorithms CDF Collaboration. Data Taking Efficiencies. 2002 2003 2004 2005. 2002 2003 2004 2005. Record 1.4 x 10 32.

rosaking
Télécharger la présentation

Data Taking Efficiencies

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. CDFPerformance and ImprovementsDetectors, Triggers, Offline, and Analysis AlgorithmsCDF Collaboration

  2. Data Taking Efficiencies 2002 2003 2004 2005 2002 2003 2004 2005 Record 1.4 x 1032 ~85% of Run IIb Upgrade Projects were commissioned with beam during this period. Initial Luminosity (1030 cm-1s-1) Data Taking Efficiency Thanks to the Accelerator Div. Detector/trigger/DAQ downtime ~5% Beam Conditions, Start/end stores ~5% Trigger deadtime ~5%: our choice 83.5%

  3. Data for Physics Recorded Data up to Aug. 23, 2005 Recorded: 950 pb-1 Physics: 620 ~ 880 pb-1 Data up to Aug. 2004 Recorded: 530 pb-1 Physics: 320 - 470 pb-1 QCD Electroweak B Top Sep-Dec ‘05 Shutdown COT Compromised Period Store Number (Aug.23,2005)

  4. Spring-Summer ’05 Highlights (Data up to Aug. 2004) Top mass l+jets Z’ in ee CDF Run II Prelim. (448 pb-1) MtopCDF = 172.2 ± 3.7 GeV ~2% accuracy Mtop: 5 papers in preparation Z’: 1 paper in preparation hep-ex/0508051 CDF Run II Preliminary 95% CL Limit - 7.9 ps-1 (355 pb-1) (Semileptonic + Hadronic) Bs Mixing pub.: wait for better results MSSM Higgs in ’s: paper submitted

  5. Run II Publication Status http://www-cdf.fnal.gov/physics/pub_run2/ • 2005 Goal: • 40 papers submitted • 2005 Status: • 20 papers - submitted (9 published, 2 accepted) • 10 papers - drafts under collaboration’s review • Results approved by CDF physics groups • Drafts approved by internal reviewers • “Godparents committee” assigned for each paper. • 27 papers - under godparents committee’s review • Results approved by CDF physics groups

  6. Current StatusandPreparation for Future

  7. CDF Detectors Performing very well. Even Run IIb Detectors! - Operational since early 2006

  8. CDF Detectors • Run IIb Upgrades: • Central Preshower Detector • Replacing with a finer segmentation system • Electron tagger, / separation • Installed fall 2004 • Electromagnetic Timing • New system for rejecting beam-halo and cosmic ray • Searches with  (e.g. GMSB SUSY, long-lived particles) • Installed fall 2004 For the future, tracking systems are our main concerns.

  9. Tracking Performance: COT and Silicon COT Gain vs. Time May 2004 Jan.2002 Aug.2005 • COT Aging - Fully Recovered • Aging due to hydrocarbons coating sense wires • Fixed by adding Oxygen • Fully recovered May 2004 • 99.7% working! • Silicon detector lifetime is a complex issue involving • Component failures • ~93% powered; ~84% working + 4% recoverable in offline • Secondary vertex trigger requires 4 layers: 21 out of 24 wedges • Beam incidents • lost ~2% of chips: conditions improved, but still concern • Long-term radiation damage

  10. Silicon Detectors • Radiation damage • > 90% of total radiation is due to collisions: NIM A514, 188-193 (2003) • Bias voltage scans as luminosity accumulates • Study collected charge (hits on tracks) and mean noise • Measurements agree with predictions up to 1 fb-1. • Efforts to increase the Silicon lifetime • Lowered Silicon operating temp. gradually from -6oC to -10oC. • Thermally isolated SVX from COT inert regions such that the silicon can be kept cold during COT work. Predicted Silicon Lifetime 8 fb-1 Lifetime 0 10 fb-1 20 fb-1 30 fb-1 40 fb-1

  11. Offline Software & Computing Readiness

  12. Data Reconstruction CDF Run2 Prelim. L=790 pb-1 CDF Run2 Prelim. L=790 pb-1 Data up to July 20, 2005 Ave. inv. mass at Z peak [GeV] yellow band: ±0.5% E scale Run Number (up to July 20, 2005) M(e+e-) [GeV/c2] • Recently achieved 6 week turn-around time between data taking and availability of physics-quality data with final calibrations. • This reduced resource needs (person and computing). • Reconstruction algorithms are stable since January 2005. • Incorporated Run II detector upgrades. • No major changes anticipated in the future.

  13. Data Reconstruction • CDF Production executable is fast. • ~110 million events / week • 50 streams: high pT e, , , jet, Hadronic B, J/, J/  ee, …. • The ave. executable time increases by x2.5 from Lpeak = 1x1032 cm-2s-1 to 3x1032 cm-2s-1. We have already demonstrated this capacity. • Plan to process all the data until the end of Run II at Fermilab. Number of data events written to tape by Production Farm Aug 23 - Sep 3, 2005

  14. Monte Carlo Simulation and Production • Detector simulation reaching maturity - matching data • Incorporated detector configuration changes with time • Incorporated multiple interactions for data instantaneous luminosity • Increasing access to global computing resources (GRID philosophy) to match physics needs. • Running on worldwide computing clusters - shared with LHC • ~100% of MC samples are generated outside of US. • Planning data analysis centers at remote sites • Physics analyses produced with remotely located datasets • Italian inst.s, Karlsruhe: J/ lifetime, B tagging, Single top • Worldwide computing resources transparent to physicists. • Aim to support more computing with fewer FTEs

  15. Alignments, Calibrations, Algorithms

  16. Tracking and High pT Lepton Status • COT Tracking • Alignment: wire positions aligned better than 10 m • Efficiency: 99.6% (isolated tracks), > 96% (non-isolated tracks) • Silicon Tracking • Alignment: internal - 5 m, w.r.t. COT < 10 m • Efficiency: 94% with r-, 83% with r-and z • Misidentified: 0.5% - 1.5% • High pT Electron Identification • Efficiency: 82-93%, Misidentified jets: ~10-4 • High pT Muon Identification • Efficiency: 93%, Misidentified jets: ~10-4 • Numbers are stable with time, instantaneous luminosity up to 1032 cm-1s-1.

  17. Momentum and Energy ScaleStatus p p J/+- mass vs 1/pT p / p = - 0.0010 ± 0.0001 • Understand passive material well: • see E/p tail • Momentum scale: • flat over a large pT range. • MW uncertainty due to P, E scale • Run II current(Run Ib) • : 30 (87) MeV, e: 70 (80) MeV • better than Run Ib Data MC Simulation E / p of W electrons p / p = - 0.0013 ± 0.0001 1 / pT(GeV-1) +- mass (GeV) near Upsilon

  18. Forward Tracking and Lepton Improvements • Forward leptons • Acceptance improvements (e.g. 30% for SM Higgs) • Forward tracking, Forward electrons(used for many analyses) • Forward muons: • efforts in improving triggers and algorithms Electrons without tracks  > 90% up to || < 3 Electrons with tracks e.g. W charge Asym. Tracks Efficiency ||

  19. B and Tau Tagging: Status / Improvements 3rd generation is important: Top, Higgs, SUSY, … Hadronic Tau Better algorithms: Neural Network Sec. Vertex B Tagging Forward Evis(GeV) Jet mis-id (%) efficiency (%) Loose (1.8% mistag) Tight (0.6% mistag) Ejet (GeV) • Ongoing efforts: • Increasing efficiency / reducing fake rate (better algorithms) • increasing acceptance (forward region)

  20. EJet Scale & Resolution: Status / Improvements 0.2 1.0 0 Mhiggs = 120 GeV No corrections 17% resolution 0 50 100 150 200 250 0.2 1.0 0 Scale Corrections Resolution Improvements 0 50 100 150 200 250 • Jet energy scale uncertainty: • precision meas.s (Mtop), searches(Higgs) • now ~2.5% uncertainty for jets in top decays • further improvements: • generators, higher order QCD • better scale for ET > 100 GeV region • complete by end of this year • Jet energy resolution: • searches (Higgs, …) • currently 17%, goal 10-11% (jets from MW =120GeV) • further improvements: • combine track, calorimeter Info: 2% • expand cone size: 2% • b-jet specific corrections:1-2% • better algorithms: 1-2% • complete by spring 2006 10% resolution bb invariant mass (GeV)

  21. Algorithms for Bs mixing: Status / Improvements • Complex meas.s involving many detector systems and analysis tools • Triggering: optimized SVT algorithms • Reconstruction modes • Currently adding Bs Ds 3 (x1.5) • Will add Bs Ds* by summer 2006 • Currently adding Bs Dsl sample using SVT 2-track triggers (x2) • Tagging (D2) • e, , jet charge (1.5%) • Same-side K tagging in progress (~2%) • Decay length resolution • Improving vertex resolution by 10~20% for larger ms • Implementing into analysis by fall 2005 • Reducing systematic uncertainties by fall 2005 • Hadronic modes - better calibration in flavor tagging • Semileptonic modes - better understanding of backgrounds

  22. High Lum. Impact on Reconstruction / Physics Understanding Tracking, B-tagging Performance at 3 x 1032 cm-2s-1 < # of interactions > ~ 10 Data vs primary vertices vs bunch-by-bunch lum. MC + multiple interactions Work in progress Developing Analysis Techniques W Mass Tracking performance vs. # vertices Z  ee events 7 8 9 10 0.2 x 1032 cm-2s-1 1.0 x 1032 cm-2s-1 2.0 x 1032 cm-2s-1 3.0 x 1032 cm-2s-1 MTW pTlepton

  23. Run IIb Trigger / DAQ Upgrades • Instantaneous Luminosity: 2 x 1032 cm-2s-1 (IIa)  3 x 1032 cm-2s-1 (IIb) • Ave # of interactions = 10, more hits / event • Level-1: Tracking Triggers • low pT tracks + hits from extra interactions mimic high pT tracks • Lower purity  higher Level-1 trigger rate • Upgrade: 2D to 3D tracking  high purity and lower rate • Level-2: Decision System and Secondary Vertex Trigger • Upgrade: Lower processing time  higher bandwidth, more flexible • DAQ, Level-3 computing, Data Logging: • Upgrade: higher bandwidth + event size increase

  24. DAQ / Trigger Specifications • Run IIa Level-1 Accept not achieved due to • higher than specified Silicon Readout and Level-2 Trigger execution times. • ** Assume ~5% from readout and ~5% from L2 processing

  25. Run IIb Project Status • Trigger and DAQ Upgrades • Level-1 Track Trigger (XFT): • Add z (stereo) info for 3D tracking - In production • COT TDC modification to achieve L2 rate of 1000 Hz (readout time) • 12 out of 20 crates are operational. • Level 2 decision system: faster,flexible - operational since April 2005 • Level 2 Silicon Vertex Trigger (SVT) • Faster - 3 step upgrade: the first 2 steps are operational. • Event Builder: operational since August 2005 • Level-3 Computing Farm • 1st procurement(64 PCs) in place-replace current system in Nov’05 • 2nd procurement(64 PCs) - ~Jan.06 • Data Logging (20 MB/s 60 MB/s) • 1st step operational (~35MB/s), complete by end of 2005 Installation & commissioning parasitically with minimal impact on operations.

  26. Run IIb Upgrade Status • Very successful so far: • 85% complete • Will finish by early 2006 • Upgrade success due to: • Highly successful Run IIa detector/trigger design & operation • Carefully targeted to specific high luminosity needs • This allowed for incremental and parasitic implementation and commissioning with minimal impact on operations. • Some cases (e.g. COT TDC), instead of building new detectors, we gradually improved the systems.

  27. Physics Triggers for 3 x 1032 cm-2s-1

  28. Extrapolation to 3 x 1032cm-1s-1 Average luminosity (36 bunches) Bunch-by-bunch luminosity • Triggers are sensitive to multiple interactions. • Measure cross section vs # of primary interaction vertices. • Calculate cross sec vs lum. using Poisson distribution of # of primary vertices. • Good agreement with bunch-by-bunch data. Level-2 high pT electron Level-2 high pT muon (0.6 < || < 1.1) a highly non-linear behavior Stereo confirmation of tracking triggers trigger rate = cross section x L at 3 x 1032 cm-2s-1 ~3% of Level-2 bandwidth ~50% of Level-2 bandwidth. Reduce to ~10 % with XFT upgrade

  29. Extrapolation to 3 x 1032cm-1s-1 Cross sections of high pT triggers (high pT e,,,jet,ET) with Level-1 upgrade Covers W, Z, Top, WH, ZH, HWW, SUSY (partial), LED, Z’ ~1/3 of Level-2 bandwidth at 3x1032 cm-2s-1: studying further improvements Studied triggers for “full” high pT physics program: ~2/3 of bandwidth. Aim for 50% of bandwidth

  30. Physics Triggers at 3 x 1032 cm-2 s-1 • Trigger Table in current operations is good to ~1.5 x 1032 cm-2s-1 • Kept improving as luminosity increases. Significant efforts! • Trigger Table for ~3 x 1032 cm-2s-1 • high pT physics program - aim for 50% • The remaining bandwidth will be given to B physics • Strategy: Developed high purity triggers for high luminosity while keeping inclusive heavy flavor triggers at low luminosity. • Level-1,2 upgrades improve purity, reduce processing time. • Other tools being implemented: • vetoing high multiplicity events • Final decision on the trigger composition • based on physics priority and purity of triggers • Straw Trigger Table ready by October 2005. L(1032) Lpeak = 3 x 1032 In 3.5 hours, L < 1.5 x 1032 66% 34% hours

  31. Concluding Remarks: CDF Strategies

  32. Concluding Remarks • CDF experiment is operating well. Better than ever! • Typical data taking efficiencies in the mid 80%’s with increasing inst. Luminosity and Run IIb commissioning • All detectors are in excellent conditions • Stable offline software • Established fast calibrations, data processing scheme • Good detector simulation • MC production at remote sites • Challenging ahead… • x2 higher instantaneous luminosity • x8 higher integrated luminosity • Resources going down • CDF Strategies in preparation for the future • Planning ahead: we have been identifying those areas that need further development and are beginning to address them immediately. Goal is to complete the work by early 2006.

  33. Concluding Remarks (cont.) • To be done by the end of 2005 or early 2006 • Complete Run IIb upgrades (~85% currently operational) • Expected to be done by the end of this year. • Physics trigger table up to 3 x 1032 cm-2s-1 being prepared. • Straw Trigger Table by October 2005 • Tuning simulation • Need one more iteration for analyses with L > 1 fb-1 • Calibrations and algorithms that require large resources • Reducing Jet energy scale uncertainty • Need one more iteration for analyses with L > 1 fb-1 • Implementing algorithms for better Jet energy resolution • Improving forward tracking and B tagging • Preparing reconstruction algorithms for high inst. Lum. • Tracking • B tagging

  34. Concluding Remarks (cont.) • Looking forward to Summer 2006 conferences • Results with x3 increase in statistics over Summer 2005 • Report on > 10 x Run I Luminosity !! • The upcoming years will be an exciting time with increasing statistics • Discovery through searches • Discovery through precision experiments • CDF Experience: • With ~4 pb-1, Top limits set • With ~20 pb-1, Evidence paper out! • With ~65 pb-1, Discovery paper out! • Hoping for new discovery with ~1 fb-1 • New physics could appear with every factor of 3~4. • CDF is committed to operating well and analyze the data through 2009.

  35. Back-up Slides

  36. Upgrading Silicon Vertex Trigger (SVT) Run 203624 Sep.1 2005 3 step upgrade: first two steps complete and operational As expected, core of timing stays the same, but tails are significantly reduced. Bigger improvements expected later. Run 203325 Aug.26 2005 SVT processing time (s)

  37. Future B Triggers • Current B triggers • High bandwidth tracks and leptons at L1, followed by SVT at L2. • What we’ve done so far • Developed high purity triggers for high lum, while keeping inclusive heavy flavor triggers at low lum. • 2 tracks - vetoing high multiplicity events • Transverse mass requirement • 2 tracks +  • For the future • XFT (L1) and SVT (L2) will improve purity and reduce L2 processing time. • Multi track combination - dedicated+track trigger. • Kinematic variable requirements with stereo information at L2. • Upgraded L2 decision is extremely flexible (firmware). • B program will not be fully active at peak lum, but we will continue to accumulate large hadronic B samples throughout the life of CDF.

More Related