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Search for neutral MSSM Higgs bosons decaying to ? pairs in pp collisions at 1.96 TeV (CDF)

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No signal evidence observed for mA = 90 through 250 GeV/c2. 10/23/06 ... This search also excluded regions of higher tan. Results similar to those of D0 ... – PowerPoint PPT presentation

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Title: Search for neutral MSSM Higgs bosons decaying to ? pairs in pp collisions at 1.96 TeV (CDF)


1
Search for neutral MSSM Higgs bosons decaying to
? pairs in pp collisions at 1.96 TeV (CDF)
  • Jessica Leonard
  • Oct. 23, 2006
  • Physics 835

2
MSSM Higgs
  • How do particles have mass?
  • SM Higgs mechanism
  • Problems with SM Higgs may be solved in MSSM
  • Five Higgs in MSSM 2 charged, 3 neutral
  • This paper deals with neutrals (?)
  • 1 CP-odd A
  • 2 CP-even h (lighter), H (heavier)
  • MSSM parameters
  • mA
  • tan ? vu/vd, where vu, vd are vevs of neutral
    Higgs that couple to up- and down-type fermions

3
MSSM Higgs
  • For large tan b, one CP-even Higgs has similar
    mass, couplings to A
  • Dominant ? production mechanisms
  • Gluon fusion
  • bb fusion
  • Dominant decay modes for A, mass-degenerate
    CP-even state
  • ? -gt bb (90)
  • ? -gt ?? (10)

4
The search at CDF
  • Tevatron CM energy 1.96 TeV
  • Data collected at CDF II between 2002-04
  • Integrated luminosity 310 pb-1
  • ? -gt ?? for 90 lt mA lt 250 GeV/c2
  • One ? -gt lepton neutrinos (?e, ??)
  • Other ? -gt hadrons neutrino (?had)

5
CDF detector
?-ln(tan(?/2))
6
Event selection
  • For the ? -gt ?? search, each event must contain a
    lepton candidate (e or ?) and hadrons consistent
    with a ? decay.
  • Pre-select with a lepton plus track condition
  • Lepton and track must both point into central
    cal.
  • Must have azimuthal separation of gt 10o
  • e/? determination
  • Electrons only deposit energy in EM calorimeter
  • Muons seen in muon chambers outside cal.
  • Momentum of neutrinos missing transverse energy

7
Event selection
  • Hadron reconstruction
  • Energy from ? decays are deposited in a small,
    contiguous region
  • Four-momentum of this jet determined from tracks
    of charged particles and energies of ?0s within
    signal cone
  • Particles in a ring outside the signal cone must
    have very low transverse energy (lt 1 GeV total).
    This isolation cuts out quark and gluon jets.

8
Event selection
  • Hadron reconstruction
  • The jets must have 1 or 3 tracks (charged
    particles), and sum of charges ?1
  • Invariant mass must be lt 1.8 GeV/c2 ( m?)
  • Require (Ecl/Psigtrk)(0.95-f)gt0.1 to reject
    electrons
  • Ecl value of energy deposit in the calorimeter
  • f ratio of electromagnetic to hadronic energy
  • Psigtrk scalar sum of track momenta in signal
    cone
  • Require ETcl gt 15 GeV to reject muons

9
Event selection
  • Hadron reconstruction efficiency
  • 38 at pThad 15 GeV/c
  • 46 at pThad gt 25 GeV/c
  • Probability of misidentifying quark or gluon jet
  • 1.5 at ETjet 20 GeV
  • 0.1 at ETjet 100 GeV

10
Monte Carlo Simulation
  • Event generation PYTHIA, with CTEQ5L PDFs
  • Tau decays TAUOLA package
  • Detector response GEANT-based model

11
Backgrounds
  • Dominant background Z/? -gt ??
  • Second-highest fake ?s (misidentified quark
    or gluon jets) from processes like di-jet,
    multi-jet, Wjets, ?jets
  • Third Z/? -gt ll, WW, WZ, ZZ, tt
  • Background contributions determined by Monte Carlo

12
Eliminating backgrounds
  • Cut out low-energy multi-jet backgrounds
  • Each e/? candidate must pass pT threshold of 10
    GeV/c
  • Each ?had candidate must pass pT threshold of 15
    GeV/c, must also have opposite charge
  • Require pTlpThadETmiss gt 50 GeV

13
Eliminating backgrounds
  • Cut out Wjets backgrounds
  • Define
  • p?vis (pl phad) ? ?
  • p?ETmiss ETmiss ? ?
  • Require p?ETmiss gt 0.6p?vis - 10 GeV/c
  • Removes 85 Wjets events, keeps 95 of signal
  • Cut out Z -gt ll decays with misidentified lepton
    reject events with lepton 1-prong ?had
    invariant mass within 10 GeV/c2 of Z mass

14
Signal Acceptance
  • For mA 90 GeV/c2, combined acceptance for
    ?e?had and ???had channels is 0.8
  • For mA 250 GeV/c2, combined acceptance is 2.0

15
Uncertainties
  • Systematic uncertainties for particle ID
    efficiency ?had 3.5, e 1.3, ? 4.6
  • Uncertainties in trigger efficiency ?e?had 2.1,
    ???had 1.4
  • Jet -gt ? misidentification 20 (3 bg. overall)
  • Uncertainty in signal acceptance
  • Due to event-level cuts lt 2
  • Due to PDFs 5.7

16
Expected events from SM
  • Number of expected standard model events passing
    all cuts
  • 496?5(stat)?28(sys)?25(lumi)
  • for a range of 438 to 554 events
  • Breakdown
  • 405 from Z/? -gt ??
  • 75 from jet -gt ? misidentification
  • 16 from all remaining background sources

17
Data
  • 487 observed events
  • Reconstructed the mass (mvis) for each event
    invariant mass of visible tau decay products and
    ETmiss
  • NOTE This is incorrect!
  • Binned the data to compare with background and
    hypothetical Higgs data
  • No signal evidence observed for mA 90 through
    250 GeV/c2

18
Example plot mA 140 GeV/c2
19
Exclusion limits
20
Excluded regions
  • Plotted excluded regions in parameter space for
    four situations
  • mhmax vs. no-mixing
  • ? gt 0 and ? lt 0

21
Excluded regions
22
Conclusions
  • LEP excluded mA lt 93 GeV/c2, higher mA for small
    tan ?
  • This search also excluded regions of higher tan ?
  • Results similar to those of D0
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