1 measurements at 8 tev of ttbar events with additional particles in the final state boris mangano...

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1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration

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Page 1: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

page 1

Measurements at 8 TeV of TTbar events

with additional particles in the final state

Boris Mangano (ETH Zürich)

on behalf of the CMS collaboration

Page 2: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 2

Outline

TTbar plus what?

- TTbar+jets

- TTbar+BBbar

- TTbar+V:

o TTbar+gamma

o TTbar+Wo TTbar+Z

8TeV results released during the last 12 months

Were these processes seen also at 8TeV ?

new results

PAS TOP-12-041

PAS TOP-13-010

PAS TOP-13-011

8 TeV

TOP-12-018

PAS TOP-12-024

TOP-12-014

7 TeV

Page 3: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 3

Motivation

TTbar plus what?

- TTbar+jets

- TTbar+BBbar

- TTbar+V:

o TTbar+gamma

o TTbar+Wo TTbar+Z

About ½ of TTbar events contain extra jets with |h| < 2.4, pT>30 GeV. Possibility to test higher order QCD calculations.

Irreducible non-resonant background for ttH (H->bb) analysis.

Potential to verify if couplings to the top quark are compatible with SM or altered by BSM effects.

Page 4: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 4

tt+jets @ 8TeV (19.6 /fb)PAS TOP-12-041Event selection:

- Dilepton OS events (el and mu)- For same-flavour pairs, Z-veto

and require MET- N-jets >=2- N-bjets >=1

Unfolding:- cross-section in N-jets bins is

presented at particle level

Extra jets definition:- Kinematic reconstruction

method to identify b-jets from ttbar decay.

- Other extra jets are then analysed

Main source of uncertainty:Up to 20% uncertainty from jet-energy-scale and signal model uncertainties.

Page 5: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 5

The whole is greater than the sum of its parts (Aristotle)

MC@NLO + Herwig does not generate sufficiently large jet multiplicities.

tt+jets @ 8TeV (19.6 /fb)

Page 6: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 6

The whole is greater than the sum of its parts (Aristotle)

Leading extra jet pT (GeV)

tt+jets @ 8TeV (19.6 /fb)

Second Leading extra jet pT (GeV)

These distributions are at reconstruction level

Page 7: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 7

PAS TOP-13-010Event selection:- Dilepton OS events (el and mu)- For same-flavour pairs, Z-veto and

require MET- N-jets >=4- N-bjets (tight) >=2

tt+bb@ 8TeV (19.6 /fb)

Main source of uncertainty:20-25% total uncertainty. Mostly from uncertainties in b-tagging discriminator templates.

Normalization of simulated samples:- Performed by means of a fit to the

measured b-tagging algorithm discriminator.

- Templates for different tt+X samples (including tt+bb signal) are taken from simulation.

Page 8: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 8

The whole is greater than the sum of its parts (Aristotle)

First additional jet Second additional jet

Simultaneous template fit of two data distributions

tt+bb@ 8TeV (19.6 /fb)

Page 9: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 9

The whole is greater than the sum of its parts (Aristotle)

Factor 0.38 to account for difference in selection efficiency between ttbb and ttjj (from simulation)

Cross-section ratio at particle level:

tt+bb@ 8TeV (19.6 /fb)

using again selection efficiencies from simulation

Page 10: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 10

PAS TOP-13-011Event selection:

- one isolated central m with pT > 26 GeV - Veto on extra leptons- N-jets >=4, with pT > 55, 45, 35, 20 GeV- N-bjets >=1- One central photon ET > 25 GeV- DR (photon,muon) > 0.7

tt+gamma @ 8TeV (19.7 /fb)

Main source of uncertainty:20-25% total uncertainty from modelling of the background template.

Signal extraction:

- Template fit of charged-hadron-isolation discriminant distribution in data.

- Templates for signal and misidentified photons from simulations.

Page 11: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 11

tt+gamma @ 8TeV (19.7 /fb)

N-1 plots for some of the observables used to select the signal photons.

Page 12: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 12

The whole is greater than the sum of its parts (Aristotle)

tt+gamma @ 8TeV (19.7 /fb)

Fit of distribution of thecharged-hadron-isolation discriminant

Inclusive ttbar cross section (TOP-12-017)

Page 13: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 13

ttW and ttZ @8TeV (19.5 /fb)

- Both ttW and ttZ processes are very rare and the measurement of their cross sections can be used to test the internal consistency of SM.

TOP-12-036

pre-print to be released in the next days

- ttZ production allows the probe of tZ coupling.

Page 14: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 14

ttW in same-sign dilepton

Signal region definition:- Tight prompt-lepton selection- same-sign dilepton (el or mu)- third lepton vetoed only if it makes a

Z-candidate- N-jets >= 3- N-bjets >=1- lepton pT>40 GeV and HT > 155 GeV

Analysis type:counting experiment

Against misidentified prompt leptons and ttbar background

Against WZ and other diboson processes. Remove overlap with ttZ analysis.

Final optimization against ttbar background

Page 15: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 15

ttW in same-sign dileptonDominant background:

- ttbar with misidentified leptons is estimated from data. Uncertainty is about 50%.

Other backgrounds:

- ttZ, WZ and other rarer processes are estimated from simulations.

- Z+jets with mis-measured lepton charge estimated from data

Six signal regions to exploit larger S/B in plus-plus channels.

Page 16: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 16

ttZ in trilepton

Analysis type:counting experiment

Signal region definition:- Three tight leptons (el or mu)- Two same-flavour opposite-sign

making a Z-candidate- N-jets >= 4- N-bjets (loose) >=2 & N-bjet

(medium) >=1

Against misidentified leptons and ttbar background

Against WZ and other diboson processes. Remove overlap with ttW analysis.

Page 17: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 17

ttZ in trileptonDominant background:

- non-top-quark background processes with b-jets from ISR. Uncertainty is about 50%.

Other backgrounds:

- TTbar with misidentified leptons is estimated from data.

- Rarer, and irreducible, SM processes estimated from simulation

Only one signal region is used for the statistical interpretation of the data

Page 18: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 18

ttZ in four-lepton

Analysis type:counting experiment

Signal regions definition:- Four tight leptons (el or mu)- Two same-flavour opposite-sign

making a Z-candidate- Veto on second Z-candidate- N-bjets =1- N-bjets >1

Against WZ and lepton misidentification

Two non-overlapping signal regions

Against ZZ background

Page 19: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 19

ttZ in four-leptonBackgrounds:

- ZZ(*) in four leptons is estimated from MC

- Z+X events with misidentified leptons

Limits and benefits of this channel:

- statistically limited

- Large S/B ratio

Page 20: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 20

ttV (V = W or Z)

Results in agreement with SM predictions:

cross section ttW = 206 ± 23 fbcross section ttZ = 197 ± 25 fb

Numbers from MG5_aMC@NLO. They are compatible with first NLO calculations from MCFM and PowHel.

Page 21: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 21

Summary

TTbar plus what?

- TTbar+jets

- TTbar+BBbar

- TTbar+V:

o TTbar+gamma

o TTbar+Wo TTbar+Z

8TeV results released during the last 12 months

PAS TOP-12-041

PAS TOP-13-010

PAS TOP-13-011

TOP-12-036

pre-print to be released in the next days

New Results

Page 22: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

Latsis Symposium 2013 page 22Boris Mangano

Backup slides

Page 23: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 23

ttV (V = W or Z)

Page 24: 1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris

LHCP 2014Boris Mangano page 24

The whole is greater than the sum of its parts (Aristotle)

tt+jets