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Search for T, T e e,

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Particles predicted by the Low Scale Technicolor Model. TCSM - Eichten, ... Phenomenology ... Low Scale Technicolor Phenomenology: color singlet vectors ... – PowerPoint PPT presentation

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Title: Search for T, T e e,


1
Search for ?T, ?T! e e-, ??-
Search for ?T, ?T! ee- Greg Landsberg Meenakshi
Narain Search for ?T, ?T ! ??- John
Butler Ryan Hooper
  • Particles predicted by the Low Scale Technicolor
    Model
  • TCSM - Eichten, Lane and Womersley
  • TCSM2 - K. Lane hep-ph/9903372

2
Low Scale Technicolor Phenomenology
  • Technicolor Models requiring large number of
    technifermion doublets
  • Topcolor-assisted Technicolor
  • Walking Technicolor
  • Low Scale Technicolor Phenomenology
  • color singlet vectors (200 400 GeV)
  • produced in pp collisions
  • Decays
  • color-singlet scalars
  • lightest technihadrons pT0 pT/-
  • Decays
  • Cross section for depends on two main model
    parameter choices
  • Difference in the ?T and ?T mass
  • The mass parameter MVMAMT, which controls the
    rate of ?!??T
  • wT ? gpT r0T ?pT pT r_T ? pT
    pT
  • ? gZ ?WpT , ZpT ? WpT,ZpT
  • ? 3pT ?WW ? WZ
  • ? f f, g g ? f f, g g

pT ? ff,gg (pT0 ? bb, pT/- ? bc dominate)
3
RunI Results
  • PRL analysis by Heintz and Narain

Difference in ?T and ?T mass
Vary mass parameter MVMAMT
4
Search for Technicolor to Dielectrons
  • Search for rT/wT ? ee- as a bump/excess at high
    dielectron mass
  • Analysis based on Landsberg, Perez LED and Z
    searches
  • Use identical cuts ? same data events and same
    background estimates
  • Intrinsic widths of ?T,?T are about 0.5 GeV
  • Thus resonance width dominated by detector
    resolution
  • Optimized mass dependent cut window for this
    particular search

5
Dielectron Analysis
6
Dielectron Analysis
Blue curves m(?T)-m(?T)60 GeV Magenta
curves m(?T)-m(?T)100 GeV
For a given set Uppsermost curve MT500
GeV Middle curve MT200 GeV Lowermost curve MT
100 GeV
7
Limits from dielectron Channel
  • 95 C.L.
  • m(?T ,?T)-m(?T)60 GeV
  • m(?T) gt 367 GeV for MT 500 GeV
  • m(?T) gt 340 GeV for MT 100 GeV
  • m(?T ,?T)-m(?T)100 GeV
  • m(?T ,?T) gt 355 GeV for MT 500 GeV
  • m(?T ,?T) gt 240 GeV for MT 100 GeV
  • Compare to RunI
  • m(?T ,?T)-m(?T)60 GeV
  • m(?T ,?T) gt 250 GeV for MT 100 GeV
  • m(?T)-m(?T)100 GeV
  • m(?T ,?T) gt 230 GeV for MT 400 GeV
  • m(?T ,?T) gt 206 GeV for MT 100 GeV

8
Search for Technicolor to Dimuons
  • Search for rT/wT ? mm- as a bump/excess at high
    mm mass
  • Motivation identical to the dielectron search
  • Analysis based on Ryan Hoopers LED and Z
    searches (DØ notes 4229 4230) updated for a 250
    pb-1 data set
  • Use identical cuts ? same data events and same
    background estimates
  • pT gt 15 GeV
  • Cut on (h1 h2) to remove cosmics
  • hdet lt 2
  • TC mass dependent cut window

9
Search for Technicolor to Dimuons
  • Acceptance Efficiency
  • Pythia 6.220 implementation of TCSM
  • Generated 100k events for each mass point
  • pm smeared using pmcs prescription (DØ note 4297)
  • Use Ryans
  • Map in h-f for Acce
  • pT re-weighting procedure
  • 1 overall error assumed
  • Results
  • For MT 100 GeV and (rT - pT) 60 GeV, exclude
    masses lt 240 GeV
  • Exceeds the Run I ee limit
  • First in dimuons for DØ
  • Combine with the ee limit

10
Conclusion
  • We have performed a search for ?T, ?T! e e-,
    ??-
  • We have extended the limit significantly in the
    dielectron final state. The best results so far.
  • Sent to group/EB for review
  • We have a new analysis in the dimuon final state
  • We combined the limit for the two final states
  • Will be writing this up shortly and sending to
    the group/EB for review.
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