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
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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


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SLIDE 1

Top squark search in the 1-lepton channel with CMS

GDR Terascale October 30th, 2013 Alexandre Aubin

IPHC, Strasbourg

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SLIDE 2

Context

Super-symmetry

  • Standard model extension
  • Boson ↔ fermion symmetry
  • Provides dark matter candidate

(R-parity conserved)

  • Solves the hierarchy problem

Why top squarks ?

  • "Natural" SUSY (m˜

t ∼ 1 TeV) 2

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SLIDE 3

Context

Direct stop pair production two decay modes considered, same final state pp → ˜ t˜ t∗ → bbWW + ˜ χ0 ˜ χ0 Assumptions

  • Simplified SUSY models

reduces complexity to 2-3 parameters

  • BR = 100%
  • ˜

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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SLIDE 4

Selection

pp → ˜ t˜ t∗ → bbWW + ˜ χ0 ˜ χ0 → ℓ + qqbb + νℓ ˜ χ0 ˜ χ0 Pre-selection

  • 1 lepton (e/µ)
  • ≥ 4 jets, ≥ 1 b-tag
  • MET ≥ 100 GeV
  • second-lepton vetos

(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

  • W (→ ℓνℓ) + jets
  • rare (diboson, triboson, t¯

t + V , Drell-Yan)

Selected t¯ t → ℓℓ events

4

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SLIDE 5

Discriminating variables

M W

T2

MW

T 2 = min

{ my consistent with : [

  • pT

1 +

pT

2 =

Emis

T

, p2

1 = 0, (p1 + pl)2 = p2 2 = M2 W ,

( p1 + pl + pb1 )2 = (p2 + pb2)2 = m2

y

]}

5

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SLIDE 6

Discriminating variables

Hratio

T Hratio

T

= Hsame side as MET

T

Htotal

T

= ∑

MET side pT (jet)

∑ pT (jet)

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SLIDE 7

Discriminating variables

min∆Φ

min∆Φ = min {∆φ(MET, j1), ∆φ(MET, j2)}

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SLIDE 8

Discriminating variables

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

  • n-shell t

leading b-tagged jet pT

  • ff-shell t

X ∆R(ℓ, leading b-tagged jet) X lepton pT

  • ff-shell W
  • Cut & count (cross-check)
  • Boosted decision trees (primary)
  • Different regions ↔ specific kinematics

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SLIDE 9

Background estimation

Key points

t → ℓℓ modelization

  • MT tail control

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SLIDE 10

Background estimation

CR-2ℓ

  • Strong dependence to ISR/FSR description
  • Agreement with the data is okay

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SLIDE 11

Background estimation

CR-0b

  • MT tail underestimated by MC for W+jets
  • Correction with a scale-factor = 1.2 ± 0.3

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SLIDE 12

Results

˜ t → t˜ χ0

⇒ no excess is observed

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SLIDE 13

Results

˜ t → b˜ χ±

⇒ no excess is observed

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SLIDE 14

Interpretation

˜ t → t˜ χ0 ˜ t → b˜ χ±

Hypothesis reminder

  • Signal is ˜

t pair production only

  • Unpolarized tops (see next slide)
  • BR is 100% (see back-up)

Results also available for m ˜

χ± = 0.25m˜ t + 0.75m ˜ χ0

m ˜

χ± = 0.75m˜ t + 0.25m ˜ χ0

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SLIDE 15

Interpretation

˜ t → t˜ χ0 ˜ t → b˜ χ±

  • Polarization effects affects signal acceptance

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SLIDE 16

Perspectives

  • Other analysis providing complementary results
  • Ongoing combination with 0ℓ and 2ℓ channels
  • 14 TeV projections predicts 5σ discovery potential up m˜

t ∼ 750-950

GeV

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SLIDE 17

Conclusion

  • Hot topic for SUSY searches and naturalness constrains
  • Analyzed the full 8 TeV data recorded by CMS. BDT probes top

squarks masses up to 650 GeV.

  • Natural SUSY far to be ruled out
  • Ongoing combination with 0-lep and 2-lep channels, and looking

forward to the 13-14 TeV. Thank you for your attention, stay tuned !

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SLIDE 18

Back-up

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SLIDE 19

ATLAS results

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SLIDE 20

Kinematic variables

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SLIDE 21

Signal regions

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SLIDE 22

BDT and cut & count

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SLIDE 23

Results (event yields)

˜ t → t˜ χ0 ˜ t → b˜ χ±

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SLIDE 24

Results (BR variation)

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SLIDE 25

Systematics

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