Search for FCNC in top-quark events
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Search for FCNC in top-quark events
Markus Cristinzianion behalf of the ATLAS Collaboration
University of Bonn & CERN
06 July 2012
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M. Cristinziani - Search for FCNC in top-quark events
Flavour-changing neutral currents
FCNC can be enhanced in models beyond SM
0.59% (ZEUS)3.2% (D0)
0.02-0.39% (D0)
Observed limits
Top quark decaysin Standard Model
BR ~100% in SM BR ~10-14 in SMGIM mechanism
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M. Cristinziani - Search for FCNC in top-quark events
Two searches for FCNC
t→qg• Search in qg→t→blν• Single top production
t→qZ• Search in tt → qZ bW → qll blν• Final state with three leptons
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M. Cristinziani - Search for FCNC in top-quark events
Search for FCNC in single top-quark production (2.05/fb)
Phys. Lett. B 712(2012) 351, published 12-Jun-2012
One lepton (pT>25 GeV)One jet (pT>25 GeV), b-taggedET
miss > 25 GeVmT
W + ETmiss > 60 GeV
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M. Cristinziani - Search for FCNC in top-quark events
Control sample and background estimate
Background estimation• Strategy as for single top
t-channel measurement• W+jets
- simulation and control region• QCD multijets
- templates with jet-electrons Signal efficiency 5.5%
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M. Cristinziani - Search for FCNC in top-quark events
Analysis strategy Signal characteristics
• pT(top) ~0 → W and b are back-to-back• p(W) large• 4x more top than anti-top quarks
Data analysis• 11 discriminating variables• Combine in a NN with 6 background templates
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M. Cristinziani - Search for FCNC in top-quark events
Result
Observed limit @ 95% C.L.• σ < 3.9 pb (2.4 pb expected)
Dominant systematics• jet energy scale• initial/final state radiation • b-tag efficiency and mistag rate
No excess found• Binned likelihood fit• Extract upper limit
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M. Cristinziani - Search for FCNC in top-quark events
Interpretation
𝜅𝑢𝑔𝑡
Λ< 6.9 ·10
−3
TeV𝜅𝑐𝑔𝑡
Λ< 1.6 ·10
− 2
TeV
BF(t→ug) < 5.7 · 10-5
BF(t→cg) < 2.7 · 10-4
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M. Cristinziani - Search for FCNC in top-quark events
Search for FCNC in top-quark decay (2.05/fb)
submitted to JHEP 01-Jun-2012, arXiv:1206.0257
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M. Cristinziani - Search for FCNC in top-quark events
Event selection strategy tt → qZ bW → qll blν
• 3 leptons (pT > 20 GeV)• 2 same flavour |m(l+l-) – m(Z)| < 15 GeV• ET
miss > 20 GeV, >= 2 jets (pT>25 GeV) 3 ID selection
• pT (1st)>25 GeV 2ID+TL selection
• 2ID + ‘track lepton’, pT (TL)>25GeV
Orthogonal to 3 ID22% more acceptance
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M. Cristinziani - Search for FCNC in top-quark events
Event reconstruction and yield Minimisation of
• wrt jet-lepton combinations• pν (z) solution from ET
miss
Additional requirements• |mt – 172.5 GeV| < 40 GeV• |mW – 80.4 GeV| < 30 GeV• 1 b-tag for 2ID+TL
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M. Cristinziani - Search for FCNC in top-quark events
Background determination 3 real leptons: ZZ, WZ, ttW, ttZ
• at least three real leptons MC simulation
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M. Cristinziani - Search for FCNC in top-quark events
Background determination 3 real leptons: ZZ, WZ, ttW, ttZ
• at least three real leptons MC simulation
2 real leptons: Z+jets, tt dilepton, Wt single top, WW• loose lepton selection• Z+jets dominant: data driven method
- control regions in ETmiss vs m(ll) in bins of ET
miss
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M. Cristinziani - Search for FCNC in top-quark events
Background determination 3 real leptons: ZZ, WZ, ttW, ttZ
• at least three real leptons MC simulation
2 real leptons: Z+jets, tt dilepton, Wt single top, WW• loose lepton selection• Z+jets dominant: data driven method (others: MC simulation)
- control regions in ETmiss vs m(ll) in bins of ET
miss
≤ 1 real leptons: tt lepton+jets, W+jets, single top, multijet• data control region: three same-sign leptons• no events observed with looser selection
TL fake probabilitydetermined in bins ofpT and Nvtx
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M. Cristinziani - Search for FCNC in top-quark events
Result
Main syst. uncertainties• Diboson modeling (3ID)• Fake-TL (2ID+TL)
Final event selection• 16 events observed• 20 ± 7 expected
Limit extraction• Using CLs• Expected limit: 9.3 · 10-3
BF(t→qZ) < 7.3 · 10-3
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M. Cristinziani - Search for FCNC in top-quark events
Summary Two searches for FCNC at ATLAS with 2.05 fb-1
t→qg• Search in single top production qg→t→blν• Background determination as in single-top• Neural-network trained• BF(t→ug) < 5.7 · 10-5 and BF(t→cg) < 2.7 · 10-4
t→qZ• Search in tt → qZ bW → qll blν• Two channels used: 3ID and 2ID+TL• Background determination according to number of fake leptons• BF(t→qZ) < 7.3 · 10-3
Phys. Lett. B 712(2012) 351, published 12-Jun-2012
submitted to JHEP 01-Jun-2012, arXiv:1206.0257
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M. Cristinziani - Search for FCNC in top-quark events
Backup NN distribution pre-tagged
• good background modeling
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M. Cristinziani - Search for FCNC in top-quark events
Backup Posterior probability function
• direct sampling approach with same Gaussian shifts applied to each source, process and bin for each uncertainty
• large number of samples of syst. shifts created
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Expected Observed
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M. Cristinziani - Search for FCNC in top-quark events
Backup Systematic uncertainties for FCNC in decay
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M. Cristinziani - Search for FCNC in top-quark events
Backup 3ID and 2ID+TL contributions
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