1. motivation 2 analysis strategy€¦ · sm tttt cross-section ≈ 9.2 fb four-top-quarks...

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1 Search for four-top-quark production in final states with one charged lepton and multiple jets using √s = 13 TeV data collected with the ATLAS detector at the LHC Leonid Serkin INFN Gruppo Collegato di Udine and ICTP Trieste, Italy 1. Motivation LHC: unique window to search for BSM signatures Signal signature Representative tree-level SM Feynman diagrams 2 Analysis strategy 3. Systematic uncertainties 4. Results Classification of events into 18 independent topologies Detector- oriented Top-pair modeling Small bkg uncert. References [4] ATLAS Collaboration: ATLAS-CONF-2016-020 (2016). No significant excess of events observed [4] 5. Limits [1] C. Degrande et al., Non-resonant new physics in top pair production at hadron colliders, JHEP 1103 (2011) 125. [2] G. Cacciapaglia et al., Four tops on the real projective plane at LHC, JHEP 1110 (2011) 042. final state topology given by the decays of each W-boson (t → Wb) use largest branching fraction final state with a single electron or muon up to 10 jets and up to 4 b-tagged jets focus on the heaviest known elementary particle: top quark search for four-top-quark production with SM kinematics test BSM models: four-top-quark production via Contact Interaction [1] and from universal extra-dimensions scenarios (2UED/RPP) [2] target resolved topologies in single lepton decay channel exploit high jet multiplicity and large total sum of jet p T Background modelling main background: top-quark pair production in association with additional jets, categorised into tt + light jets, tt + cc and tt + bb events, the latter improved via NLO reweighting [3] Small contributions from tt + V/H, W/Z + jets, single top and diboson [3] F. Cascioli et al., NLO matching for ttbb production with massive b-quarks, Phys. Lett. B 734 (2014) 210. Simultaneous binned profile likelihood fit in 6 control and 3 signal regions leads to significant reduction in overall background uncertainty 9 regions validate the assumption that the tt + jets modelling extracted from control regions can be extrapolated to signal regions N normalisation, SN shape and normalisation Using 3.2 fb -1 of pp data at √s = 13 TeV SM tttt production: obs (exp) 95% CL upper limit on the SM production cross-section of 190 fb (143 fb) SM tttt cross-section ≈ 9.2 fb four-top-quarks production via contact interaction: upper limit of 148 fb (115 fb) tttt via 2UED/RPP: limit on m KK of 1.28 TeV (1.30 TeV) Event display of the most energetic event in signal region ¯ ¯ ¯ ¯ ¯ ¯ ¯ ¯ ¯ ¯ ¯ ¯ ¯ Impact of the nuisance parameters on signal strength S/B and S/√B values for each of the regions Fractional contributions of the various backgrounds in each region After fitting of the nuisance parameters to data under the background-only hypothesis Post-fit Pre-fit

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Page 1: 1. Motivation 2 Analysis strategy€¦ · SM tttt cross-section ≈ 9.2 fb four-top-quarks production via contact interaction: upper limit of 148 fb (115 fb) tttt via 2UED/RPP: limit

1

Search for four-top-quark production in final states with one charged lepton

and multiple jets using √s = 13 TeV data collected with the ATLAS detector at the LHC

Leonid Serkin

INFN Gruppo Collegato di Udine and ICTP Trieste, Italy

1. Motivation

• LHC: unique window to search for BSM signatures • Signal signatureRepresentative tree-level SM Feynman diagrams

2 Analysis strategy

3. Systematic uncertainties

4. Results

• Classification of events into 18 independent topologies

Det

ecto

r-

ori

ente

d

To

p-p

air

mo

del

ing

Sm

all

bk

g

un

cert

.

References

[4] ATLAS Collaboration: ATLAS-CONF-2016-020 (2016).

• No significant excess of events observed [4]

5. Limits

[1] C. Degrande et al., Non-resonant new physics in top pair production at hadron colliders, JHEP 1103 (2011) 125.

[2] G. Cacciapaglia et al., Four tops on the real projective plane at LHC, JHEP 1110 (2011) 042.

final state topology given by the

decays of each W-boson (t → Wb)

use largest branching fraction final

state with a single electron or muon

up to 10 jets and up to 4 b-tagged jets

focus on the heaviest known elementary particle: top quark

search for four-top-quark production with SM kinematics

test BSM models: four-top-quark production via Contact Interaction [1]

and from universal extra-dimensions scenarios (2UED/RPP) [2]

target resolved topologies in single lepton decay channel

exploit high jet multiplicity and large total sum of jet pT

• Background modelling main background: top-quark pair production in association with additional

jets, categorised into tt + light jets, tt + cc and tt + bb events, the latter

improved via NLO reweighting [3]

Small contributions from tt + V/H, W/Z + jets, single top and diboson

[3] F. Cascioli et al., NLO matching for ttbb production with massive b-quarks, Phys. Lett. B 734 (2014) 210.

Simultaneous binned profile likelihood fit in 6 control and 3 signal regions

leads to significant reduction in overall background uncertainty

9 regions validate the assumption that the tt + jets modelling extracted from

control regions can be extrapolated to signal regions

N ≡ normalisation, SN ≡ shape and normalisation

• Using 3.2 fb-1 of pp data at √s = 13 TeV

SM tttt production: obs (exp) 95% CL upper limit on the SM production

cross-section of 190 fb (143 fb)

SM tttt cross-section ≈ 9.2 fb

four-top-quarks production via contact

interaction: upper limit of 148 fb (115 fb)

tttt via 2UED/RPP:

limit on mKK of

1.28 TeV (1.30 TeV)

Event display of the most energetic event in signal region

¯ ¯

¯ ¯ ¯¯ ¯

¯

¯¯

¯¯

¯

Impact of the nuisance parameters on signal strength

S/B and S/√B values for each of the regions Fractional contributions of the various backgrounds in each region

After fitting of the nuisance parameters to data under the background-only hypothesis

Post-fit

Pre-fit