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Supersymmetry at the Tevatron

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m m. Leptonic branching are enhanced if sleptons are lighter than gauginos ... M(squark) 292GeV. 13. B-jets and missing energy ... – PowerPoint PPT presentation

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Title: Supersymmetry at the Tevatron


1
Supersymmetry at the Tevatron
  • R. Demina
  • University of Rochester

2
20 years of SUSY
  • And still, no one is prettier
  • We like the way she walks, We like the way she
    talks but
  • God damn it, where is she?

3
Outline
  • Data sets
  • Tri-leptons
  • Jets and missing energy
  • Straight up
  • With heavy flavor
  • Gauge Mediated SUSY Breaking photons with
    missing energy
  • Long-lived particles
  • Conclusions

4
Run II data taking
Presented analyses are based on pre-shutdown
data lt200pb-1
5
SUSY production at Tevatron
  • 200 pb-1
  • 1013collisions
  • 80 chargino/ neutralino ?(3l) events produced
  • 800 squark/gluino events produced
  • To control backgrounds searches based on
    signatures 3 or more physics objects


6
Tri-leptons
ee(l)
em(l)
  • Chargino/neutralino production three leptons
    and missing energy signature
  • Main challenge - weak production ? low cross
    sections
  • LEP limits are very restrictive
  • Need extremely well controlled backgrounds

(l ) isolated track e, m, t
  • Leptonic branching are enhanced if sleptons are
    lighter than gauginos

7
eelepton
175pb-1
  • 2 Electrons EM clustertrack match
  • PTgt12 (8) GeV
  • hlt1.1 (3.0)
  • Anti-Z
  • 15ltMeelt60 GeV
  • Df(ee)lt2.8
  • Anti-W?(en)g
  • gt1hit in silicon or tighter electron likelihood
  • Anti tt
  • Veto jets with ETgt80GeV
  • Anti-Drell Yan
  • Missing ETgt20GeV
  • Df(eMET)gt0.4

Potential signal
8
eelepton
  • Lepton isolated track
  • PTgt3GeV
  • Etmiss x PT(track)gt250GeV

e(signal)2-3
9
Tri-leptons
  • Summary after all cuts

Add isolated track with PTgt3 GeV
10
Combined tri-leptons
  • Run 1 cross section limit much improved
  • Soon will reach MSugra prediction (in the best
    scenario with low slepton masses)

11
Jets and missing energy
85 pb-1
  • Squarks and gluions
  • Strong production
  • larger cross section,
  • but really large instrumental backgrounds (2
    orders of magnitude over SM processes)

Final cuts Missing ETgt175 GeV HTgt275 GeV
2 jets ETgt60 (50) GeV 30ltDf(jet,MET)lt165o
  • 4 events left 2.67 expected from SM sources (Z/W
    production)
  • 17.1 event expected for M025,M1/2100GeV

12
Squarks and gluinos
  • M025GeV A00 tanb3 mlt0

M(gluino)gt333GeV Run 1 310 GeV
M(squark)gt292GeV
13
B-jets and missing energy
  • High tan(b) scenario under study sbottom is
    lighter than other squarks and gluino
  • 4b-jetsmissing energy
  • gt3jets (ETgt10 GeV)
  • Missing ETgt35 GeV
  • 1 b-tag
  • 5.6-1.4 events SM predicted - 4 observed
  • 2 b-tags
  • 0.5-0.1 events SM predicted - 1 observed

14
ggMet
185 pb-1
Missing ETgt40 GeV
  • Gauge mediated SUSY breaking at scale L
  • Gravitino LSP
  • NLSP (neutralino) ?g LSP
  • Dominant SUSY mode c20 c1

Signature 2 photons, missing energy PT(photon)gt2
0 GeV in hlt1.1 1 event survived 2.50.5
expected from SM
15
Long Live Particles!
d
  • LSP charged particle, or
  • NLSP charged particle (e.g. stop) with long
    decay time
  • Signature isolated track of a rather slow
    particle
  • Use TOF system (CDF)
  • BG prediction of 2.9 /- 0.7 (stat) /- 3.1
    (sys), with 7 observed

16
Conclusions
  • Tevatron detectors produce solid physics results
    based on datasets of up to 185 pb-1
  • SUSY limits extended beyond run 1
  • In trilepton signature
  • Missing energy and jets
  • Missing energy and b-jets
  • GMSB in diphoton final state
  • New system (TOF) used to search for long lived
    particles
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