Small Extra Dimension Graviton Detection at ATLAS - PowerPoint PPT Presentation

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Small Extra Dimension Graviton Detection at ATLAS

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Title: Small Extra Dimension Graviton Detection at ATLAS


1
Small Extra Dimension Graviton Detection at ATLAS
  • Looking at the Graviton as it decays through
    G-gtZ0 Z0 -gte-ee-e
  • Audrey Todhunter
  • Case Western Reserve University
  • Dominik Dannheim
  • Columbia University

2
The Graviton
  • Massive graviton resonances are predicted by
    models using extra dimensions
  • -resonances could be well separated in mass
  • The graviton couples universally
    (ee,??,??,??,Z0Z0, etc)
  • -Products could be detected at ATLAS
  • Analysis used the Randall-Sundrum model, which
    predicts the mass of the first resonance by
  • mn xn(k/MPl)??
  • We chose k/MPl0.01 to give resonances on the TeV
    scale

3
  • This analysis
  • pp?G?Z0Z0?ee-ee-
  • against a Standard Model background
  • qq?Z0Z0?ee-ee-
  • The branching ratio Br for Z0Z0?ee-ee- is only
    3.43.4 11.56 for this decay process

4
Signal and Background Simulation
  • -Pythia event generator
  • -mass points at 300GeV, 500GeV, 700GeV, 1TeV, and
    1.5TeV, as well background processes around each
    point
  • -want to know how well these signals can be
    detected at ATLAS? Geant4 used in a full
    simulation of the ATLAS reconstruction

5
Properties of simulated signal and background
6
Particle Selection
  • We can identify electrons by their
    characteristics detected in the EM calorimeter
    and the central tracker
  • Transverse energy eT gt 20 GeV
  • Likelihood gt 0.9 being electron rather than pion
  • 2ee- pairs in each entry
  • - best combination of particles decided by
    comparing reconstructed Z0 mass to known Z0 mass
    (91.1GeV)

7
Invariant Z0 mass from a 300GeV signal from
electron pairs closest to Z0 mass within each
interaction
8
Graviton Reconstruction
  • -electrons chosen for Z0 mass used to reconstruct
    invariant G mass
  • -signal scaled for 100 fb-1 luminosity (1 year
    running at design luminosity)
  • NEv (?Br) L
  • imposing a weight factor on the number of
    simulated events

9
Signal at 500GeV with a Gaussian fitsigma
parameter used to look at events within a mass
window of 3?
10
Signal and background added and fit
withp0e(-(x-p1)2/2p2 2 p3e(p4xp5)
11
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12
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13
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14
Potential discovery of resonances from
G?Z0Z0?ee-ee- at ATLAS
  • count number of signal and background events
    within the 3? window
  • need to have Nsiggt5v (NBG) or Nsig gt 10 for a
    statistically significant signal
  • number of events can be increased by raising
    luminosity

15
Luminosity needed for Nsiggt5v (NBG) or Nsig gt 10
L100fb-1 one year running at design luminosity
16
Conclusions
  • -for the process G?Z0Z0?ee-ee- the upper mass
    limit is slightly below 700GeV
  • -higher discovery potential at increased
    luminosity
  • -other decay channels are possible for the
    graviton which may have higher upper limits for
    detection
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