Top squark search in the 1-lepton channel with CMS
GDR Terascale October 30th, 2013 Alexandre Aubin
IPHC, Strasbourg
Top squark search in the 1-lepton channel with CMS GDR Terascale - - PowerPoint PPT Presentation
Top squark search in the 1-lepton channel with CMS GDR Terascale October 30th, 2013 Alexandre Aubin IPHC, Strasbourg Context Super-symmetry (R-parity conserved) Why top squarks ? 2 Standard model extension Boson fermion
GDR Terascale October 30th, 2013 Alexandre Aubin
IPHC, Strasbourg
Super-symmetry
(R-parity conserved)
Why top squarks ?
t ∼ 1 TeV) 2
Direct stop pair production two decay modes considered, same final state pp → ˜ t˜ t∗ → bbWW + ˜ χ0 ˜ χ0 Assumptions
reduces complexity to 2-3 parameters
χ0 and ˜ χ± are linear combination of gauginos and higgsinos focus here on 1-lepton channel (CMS-SUS-13-011, arXiv :1308.1586)
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pp → ˜ t˜ t∗ → bbWW + ˜ χ0 ˜ χ0 → ℓ + qqbb + νℓ ˜ χ0 ˜ χ0 Pre-selection
(isolated track, hadronic τ)
Signal region
Cut & count and BDT analysis after MT = mT (ℓ, MET) > 120 GeV
Backgrounds
t → ℓℓ
t → ℓ + jets, single t
t + V , Drell-Yan)
Selected t¯ t → ℓℓ events
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T2
MW
T 2 = min
{ my consistent with : [
1 +
pT
2 =
Emis
T
, p2
1 = 0, (p1 + pl)2 = p2 2 = M2 W ,
( p1 + pl + pb1 )2 = (p2 + pb2)2 = m2
y
]}
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T Hratio
T
= Hsame side as MET
T
Htotal
T
= ∑
MET side pT (jet)
∑ pT (jet)
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min∆Φ = min {∆φ(MET, j1), ∆φ(MET, j2)}
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Variable ˜ t → t˜ χ0 ˜ t → b˜ χ± MET X X MW
T 2
X X min∆Φ X X HT ratio
T
X X hadronic top χ2
leading b-tagged jet pT
X ∆R(ℓ, leading b-tagged jet) X lepton pT
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Key points
t → ℓℓ modelization
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⇒ no excess is observed
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⇒ no excess is observed
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Hypothesis reminder
t pair production only
Results also available for m ˜
χ± = 0.25m˜ t + 0.75m ˜ χ0
m ˜
χ± = 0.75m˜ t + 0.25m ˜ χ0
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t ∼ 750-950
GeV
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squarks masses up to 650 GeV.
forward to the 13-14 TeV. Thank you for your attention, stay tuned !
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