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Search for Long-Lived Particles at D Ø

Search for Long-Lived Particles at D Ø. Todd Adams Florida State University July 19, 2005. SUSY05. IPPP Durham. Tevatron. _. pp collisions at 1960 GeV detectors: D Ø and CDF. recorded luminosity ~8 times Run I. Introduction. Search for long-lived particles

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Search for Long-Lived Particles at D Ø

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  1. Search for Long-Lived Particles at DØ Todd Adams Florida State University July 19, 2005 SUSY05 IPPP Durham

  2. Tevatron _ • pp collisions at 1960 GeV • detectors: • DØ and CDF recorded luminosity ~8 times Run I SUSY05 – T. Adams

  3. Introduction • Search for long-lived particles • “stable” = doesn’t decay within the collider detector • can still decay • massive (>50 GeV) • charged particles = unique signature • SUSY models • GMSB: stau • chargino • optimize for pair production SUSY05 – T. Adams

  4. GMSB Model • stable stau: NLSP (LSP is gravitino/goldstino) • large value of Cgrav • Snowmass 2001 Model Line D SUSY05 – T. Adams

  5. Chargino Model • small (<150 MeV) mass difference between lightest chargino and lightest neutralino • stable chargino • higgsino-like or • gaugino-like SUSY05 – T. Adams

  6. Charged Massive Stable Particles(CMSPs) • Massive: >50 GeV • Slow-moving:  < 1 • Charged: large energy deposition • Bethe-Block formula • Long-lived: decays outside of muon detector • Will look like slow moving muon SUSY05 – T. Adams

  7. DØ Detector SUSY05 – T. Adams

  8. Muon System • Detects minimum-ionizing particles • Timing: speed of light particle will register at t=0 in all three layers • resolution is 2-3 ns • Three layers • Toroid between 1st and 2nd layers • CMSP’s will be out-of-time SUSY05 – T. Adams

  9. Trigger • Trigger requires two tracks in muon system • Timing issues: • trigger gate is asymmetric • allows later particles • trigger gate ranges from 20-85 ns for different layers • causes inefficiency for slower moving particles • efficiency drops as mass increases • sufficient for our mass range (60-300 GeV) SUSY05 – T. Adams

  10. Preliminary Dimuon Selection Luminosity = 390 pb-1 • muon pT > 15 GeV • matched to track in central tracker • scintillator hits in 2 of 3 layers of muon system • at least one isolated muon •  > 1.0 radians • cosmic ray muon rejection SUSY05 – T. Adams

  11. Muon Speed • Calculate speed of muon at each layer • v = d/t (v in units of c) • v from timing error • Calculate average velocity for each muon • Calculate speed 2 • Require 2 < 4 SUSY05 – T. Adams

  12. Speed Significance Data muons CMSP SUSY05 – T. Adams

  13. Backgrounds • Z/Drell-Yan is major background • no natural source of slow-moving high-pT particles • Use data to estimate background • use Z-peak events for timing distribution • use negative time events for invariant mass distribution SUSY05 – T. Adams

  14. Transverse Momentum Signal has larger pT SUSY05 – T. Adams

  15. Dimuon pT vs Significance Product • Significance product: Sig(1) x Sig(2) 60 GeV stau’s Real muon data SUSY05 – T. Adams

  16. Analysis Results • Background estimated using data SUSY05 – T. Adams

  17. stau Cross-section Limit Best limit from the Tevatron SUSY05 – T. Adams

  18. Charginos Charginos look like stau’s Use same analysis SUSY05 – T. Adams

  19. Chargino Limits Higgsino-like Gaugino-like M > 140 GeV M > 174 GeV DØ RunII Preliminary SUSY05 – T. Adams

  20. Effect of Lifetime • “Short” lifetime  decay within detector • loss of acceptance SUSY05 – T. Adams

  21. Conclusions • DØ has performed a search for charged, massive stable particles • look for slow moving particles • Set limits on stau and chargino production • best limits on chargino mass SUSY05 – T. Adams

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