Top Properties from ATLAS Chris Young (CERN), on behalf of ATLAS - - PowerPoint PPT Presentation

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Top Properties from ATLAS Chris Young (CERN), on behalf of ATLAS - - PowerPoint PPT Presentation

Top Properties from ATLAS Chris Young (CERN), on behalf of ATLAS 27th May 2020 1 / 19 Top Properties from ATLAS Chris Young (CERN), on behalf of ATLAS Introduction The Top pair cross-section at the LHC is large! - 830 pb at 13 TeV


slide-1
SLIDE 1

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS 27th May 2020

1 / 19

slide-2
SLIDE 2

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Introduction

◮ The Top pair cross-section at the LHC is large! - ∼830 pb at 13 TeV ◮ In Run II over 100 Million top–anti-top pair will have been produced in ATLAS. ◮ This gives us a large dataset to study the different properties of the top, the production mechanisms and its decay. ◮ We study the properties of all the different parts of top production, the top quark, the top decay, and the properties of the decay products... ◮ ATLAS has produced a large number of results so I will focus on a few here; LINK TO ALL RESULTS

Properties Related to Production

  • Cross-section and Kinematics
  • f the top and top+anti-top

system

  • > see talk by P. Jacka
  • Spin correlations
  • Charge asymmetry
  • Top quark polarization
  • FCNCs
  • Many more . . .

2 / 19

slide-3
SLIDE 3

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Introduction

◮ The Top pair cross-section at the LHC is large! - ∼830 pb at 13 TeV ◮ In Run II over 100 Million top–anti-top pair will have been produced in ATLAS. ◮ This gives us a large dataset to study the different properties of the top, the production mechanisms and its decay. ◮ We study the properties of all the different parts of top production, the top quark, the top decay, and the properties of the decay products... ◮ ATLAS has produced a large number of results so I will focus on a few here; LINK TO ALL RESULTS

Properties Related to Production

  • Cross-section and Kinematics
  • f the top and top+anti-top

system

  • > see talk by P. Jacka
  • Spin correlations
  • Charge asymmetry
  • Top quark polarization
  • FCNCs
  • Many more . . .

Fundamental Properties of the top quark

  • Mass
  • > see talk by M. Negrini
  • Width
  • > see talk by M. Negrini
  • Charge
  • Spin (indirectly)

3 / 19

slide-4
SLIDE 4

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Introduction

◮ The Top pair cross-section at the LHC is large! - ∼830 pb at 13 TeV ◮ In Run II over 100 Million top–anti-top pair will have been produced in ATLAS. ◮ This gives us a large dataset to study the different properties of the top, the production mechanisms and its decay. ◮ We study the properties of all the different parts of top production, the top quark, the top decay, and the properties of the decay products... ◮ ATLAS has produced a large number of results so I will focus on a few here; LINK TO ALL RESULTS

Properties Related to Production

  • Cross-section and Kinematics
  • f the top and top+anti-top

system

  • > see talk by P. Jacka
  • Spin correlations
  • Charge asymmetry
  • Top quark polarization
  • FCNCs
  • Many more . . .

Fundamental Properties of the top quark

  • Mass
  • > see talk by M. Negrini
  • Width
  • > see talk by M. Negrini
  • Charge
  • Spin (indirectly)

Properties Related to Decay

  • W-helicity measurements
  • CLFV: t->ll'q
  • FCNC: eg. t->hu, t->hc,

t->Zu, t->Zc, t->γu, t->γc

  • > see talk by K. Skovpen
  • Jet shapes and colour flow
  • Anomalous couplings
  • Many more . . .

4 / 19

slide-5
SLIDE 5

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Introduction

◮ The Top pair cross-section at the LHC is large! - ∼830 pb at 13 TeV ◮ In Run II over 100 Million top–anti-top pair will have been produced in ATLAS. ◮ This gives us a large dataset to study the different properties of the top, the production mechanisms and its decay. ◮ We study the properties of all the different parts of top production, the top quark, the top decay, and the properties of the decay products... ◮ ATLAS has produced a large number of results so I will focus on a few here; LINK TO ALL RESULTS

Properties Related to Production

  • Cross-section and Kinematics
  • f the top and top+anti-top

system

  • > see talk by P. Jacka
  • Spin correlations
  • Charge asymmetry
  • Top quark polarization
  • FCNCs
  • Many more . . .

Fundamental Properties of the top quark

  • Mass
  • > see talk by M. Negrini
  • Width
  • > see talk by M. Negrini
  • Charge
  • Spin (indirectly)

Properties Related to Decay

  • W-helicity measurements
  • CLFV: t->ll'q
  • FCNC: eg. t->hu, t->hc,

t->Zu, t->Zc, t->γu, t->γc

  • > see talk by K. Skovpen
  • Jet shapes and colour flow
  • Anomalous couplings
  • Many more . . .

Properties

  • f W-boson

from tt events

  • Measurement of universality

lepton c

♦ ✁ ✂ ✄☎ ✆ ✝ ✞♦ ✟ ✠ ✡ ♦ ✝ ♦ns

through:

N

❊ ❲ ✦

5 / 19

slide-6
SLIDE 6

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Introduction

◮ The Top pair cross-section at the LHC is large! - ∼830 pb at 13 TeV ◮ In Run II over 100 Million top–anti-top pair will have been produced in ATLAS. ◮ This gives us a large dataset to study the different properties of the top, the production mechanisms and its decay. ◮ We study the properties of all the different parts of top production, the top quark, the top decay, and the properties of the decay products... ◮ ATLAS has produced a large number of results so I will focus on a few here; LINK TO ALL RESULTS

Properties Related to Production

  • Cross-section and Kinematics
  • f the top and top+anti-top

system

  • > see talk by P. Jacka
  • Spin correlations
  • Charge asymmetry
  • Top quark polarization
  • FCNCs
  • Many more . . .

Fundamental Properties of the top quark

  • Mass
  • > see talk by M. Negrini
  • Width
  • > see talk by M. Negrini
  • Charge
  • Spin (indirectly)

Properties Related to Decay

  • W-helicity measurements
  • CLFV: t->ll'q
  • FCNC: eg. t->hu, t->hc,

t->Zu, t->Zc, t->γu, t->γc

  • > see talk by K. Skovpen
  • Jet shapes and colour flow
  • Anomalous couplings
  • Many more . . .

Properties

  • f W-boson

from tt events

  • Measurement of universality

lepton c

☛ ☞ ✌ ✍ ✎✏ ✑ ✒ ✓☛ ✔ ✕ ✖ ☛ ✒ ☛ns

through:

N

✗ ✘ ✙

Too many results to cover! Today I focus on 3 results...

  • Charge asymmetry
  • Spin Correlations between t
✚ ✛ ✜ ✢ ✣✤i-top
  • Measurement of the universality of the lepton

couplings t

✚ ✥ ✧ ★ ✚ ✩ ✚ ✣

N

✪ ✫ ✬

N

✭ ✮

A

LAS

CMS Comparison

6 / 19

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SLIDE 7

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Charge Asymmetry ATLAS-CONF-2019-026

◮ At leading order t¯ t production is charge symmetric. ◮ However, at higher orders inferference in qg and q¯ q, and EW contributions lead to

  • asymmetries. Also BSM physics can lead to enhancements!

◮ The gg initiated process remains charge symmetric to all orders and as this is the dominant production mechanism this dilutes the asymmetry significantly. . AC = N(∆|y|>0)−N(∆|y|<0)

N(∆|y|>0)+N(∆|y|<0)

∆|y| = |yt| − |y¯

t|

◮ This expresses the asymmetry between the top or the anti-top being more forward; positive values indicate the top is more forward than the anti-top.

q q q t t t q t

anti-top top

Not t

✯ ✰ ✱ ✲ ✳✵ ✶

7 / 19

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SLIDE 8

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Charge Asymmetry - Selection and t¯ t Reco. ATLAS-CONF-2019-026

◮ In the resolved analysis (boosted events removed); ◮ A BDT is used to assign the different jets to the top systems, including KLFitter, mass of the hadronic top and W, and various angular variables. ◮ The best combination is used and only events with good reconstruction according to the BDT output are retained. ◮ Boosted reconstruction to access highest kinematic regions; ◮ At high pT the hadronic top can be reconstructed as a single large-R jet with pT > 350 GeV, and the mass and τ32 is used to “tag” hadronic tops. ◮ The leptonic side is reconstructed from the E miss

T

, lepton and a R = 0.4 jet.

8 / 19

slide-9
SLIDE 9

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Charge Asymmetry - Results ATLAS-CONF-2019-026

◮ Results are presented for the inclusive value of AC; AC = 0.0060±0.0015[±0.0011(stat.)±0.0009(syst.)±0.0005(MC stat.)±0.0001(bias.)] ◮ 4σ from 0! - first evidence of non-zero charge asymmetry in t¯ t! ◮ This is in good agreement of the NNLO calculation of 0.0064 ± 0.0006 ◮ Additionally AC is also unfolded in bins of the mass of the t¯ t system and also in the absolute longitudinal boost of the t¯ t system in the z-direction, βt¯

t,z.

◮ In both variables good agreement is seen with the SM. ◮ Limits are set in an EFT based on the inclusive and mt¯

t results. 9 / 19

slide-10
SLIDE 10

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Charge Asymmetry - Results ATLAS-CONF-2019-026

◮ Results are presented for the inclusive value of AC; AC = 0.0060±0.0015[±0.0011(stat.)±0.0009(syst.)±0.0005(MC stat.)±0.0001(bias.)] ◮ 4σ from 0! - first evidence of non-zero charge asymmetry in t¯ t! ◮ This is in good agreement of the NNLO calculation of 0.0064 ± 0.0006 ◮ Additionally AC is also unfolded in bins of the mass of the t¯ t system and also in the absolute longitudinal boost of the t¯ t system in the z-direction, βt¯

t,z.

◮ In both variables good agreement is seen with the SM. ◮ Limits are set in an EFT based on the inclusive and mt¯

t results. 10 / 19

slide-11
SLIDE 11

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Spin Correlations in t¯ t

1903.07570

◮ The Standard Model predicts that top-quark pairs should be produced without polarization but with some correlation between their spin states. ◮ As the top quark lifetime is much shorter than the spin decorrelation time the spin information is directly transferred to the decay products. ◮ Simple di-leptonic t¯ t selection; 1 electron, 1 muon, + ≥ 1b-jet. ◮ The angle between the leptons (in both η and φ, but ∆φ is most sensitive) is then sensitive to the spin correlations.

11 / 19

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SLIDE 12

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Spin Correlations in t¯ t - Results 1903.07570

◮ Results are unfolded to both the parton-level and also the particle-level distributions. ◮ Leading uncertainties come from generator modeling (mainly rad. and scale). ◮ The data show slightly higher spin correlations than the predictions and this is quantified by fitting templates of fSM × xSM spin + (1 − fSM) × xNo spin, using the Powheg NLO prediction; . fSM = 1.249 ± 0.024(stat.) ± 0.061(syst.) +0.067

−0.090(theory)

◮ Higher order calculations appear to reduce, but not eliminate, this discrepancy.

12 / 19

slide-13
SLIDE 13

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Spin Correlations in t¯ t - Compare with CMSATL-COM-PHYS-2020-315

◮ CMS has also produced measurements of the ∆φ distribution using the data from 2015+2016 link. ◮ The data from the two collaborations agree well, as do the independently generated simulations. ◮ Both collaborations only used partial Run II datasets - more results to come!

13 / 19

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SLIDE 14

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Lepton Universality in W → lν

ATLAS-CONF-2020-014

◮ The universality of the coupling of the different generations of leptons to the gauge bosons is a fundamental axiom of the Standard Model. ◮ The large number of t¯ t events produced at the LHC gives an excellent sample of W-bosons to test this. ◮ This analysis looks to measure the ratio; R(τ/µ) = BR(W → τν) BR(W → µν) ◮ This has previously been measured at LEP with a 2.7σ discrepancy from the SM expectation of unity.

0.8 0.9 1 1.1 1.2

) ν

→ BR(W ) ν τ → BR(W ) ν e → BR(W ) ν τ → BR(W ) ν e → BR(W ) ν

→ BR(W

ATLAS Preliminary

UA1 UA2 CDF D0 LHCb LEP ATLAS PDG averages

Z.Phys. C44 (1989) 15-61
  • PLB. 280 (1992) 137-145
J.Phys.G 34 (2007) 2457-2544, PRL. 68 (1992) 3398-3402
  • PRL. 75 (1995) 1456, PRL. 84 (2000) 5710
JHEP 10 (2016) 030 Phys.Rept. 532 (2013) 119
  • EPJC. 77 (2017) 367
  • PRD. 98 (2018) 030001
  • 1

= 13 TeV, 139 fb s

modified

14 / 19

slide-15
SLIDE 15

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Lepton Universality in W → lν - Selection & Variables

◮ Events are selected with b-tagged jets and two leptons; triggered by an electron or muon, and with a second lepton which is a muon. ◮ The branching ratio of τ → µνµντ is well known such that we can extrapolate from; BR(W → τ(→ µνν)ν) BR(W → µν) → BR(W → τν) BR(W → µν) ◮ Events with muons from τ decays are distinguished from directly produced muons from their softer pT spectrum, and the displacement of the decay – through the transverse distance of closest appoach of the track, |d0|. ◮ The |d0| distribution for the prompt muons it taken from templates created from Z → µµ events, and the distribution for non-prompt muons is corrected using the measured resolution in the same selection.

0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 | [mm]

µ

|d 0.9 0.95 1 1.05 Data / Pred. 1 10

2

10

3

10

4

10

5

10

6

10 Events / 0.01 mm ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Signal Region <250 GeV

µ T

, 20<p µ e Post-Fit Data (top) µ Prompt (top) µ → τ (hadron decay) µ τ τ → Z Other SM processes Uncertainty

15 / 19

slide-16
SLIDE 16

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Lepton Universality in W → lν - Backgrounds

◮ The main backgrounds to the analysis are Z → µµ+jets in the di-muon channel, and muons from hadron decays. ◮ For Z → µµ+jets a fit of di-muon invariant mass distributions is used to normalize this background with the same jet requirements as the signal region. ◮ A same-sign charge selection is used to normalize the background of muons from hadron decays with simulation used to extrapolate to the different-sign charge selection.

60 80 100 120 140 160 [GeV]

µ µ

m 0.9 0.95 1 1.05 Data / Pred. 10000 20000 30000 40000 50000 Events / 2.5 GeV ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Z Normalisation Selection µ µ Post-Fit Data µ µ → Z Top Di-Boson processes Other SM processes Uncertainty 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 | [mm]

µ

|d 0.8 0.9 1 1.1 Data / Pred. 1 10

2

10

3

10

4

10

5

10 Events / 0.05 mm ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Control Region µ µ Same-sign Post-Fit Data (hadron decay) µ Top+V processes Di-Boson processes Other SM processes Uncertainty

16 / 19

slide-17
SLIDE 17

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Lepton Universality in W → lν - Fit & Results

◮ A fit is performed in 3 bins in pT x 8 bins in |d0| x 2 channels (e-µ,µ-µ). ◮ Good agreement is seen in the fitted distributions. ◮ The fitted value of R(τ/µ) is found to be; . R(τ/µ) = 0.992 ± 0.013 [±0.007 (stat) ± 0.011 (syst)] ◮ The most precise measurement to date (by a factor 2) and the SM prevails.

0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 | [mm]

µ

|d 0.9 0.95 1 1.05 Data / Pred. 1 10

2

10

3

10

4

10

5

10 Events / 0.01 mm ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Signal Region <20 GeV

µ T

, 10<p µ µ Post-Fit Data (top) µ Prompt (top) µ → τ (hadron decay) µ µ µ → Z τ τ → Z Other SM processes Uncertainty 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 | [mm]

µ

|d 0.9 0.95 1 1.05 Data / Pred. 1 10

2

10

3

10

4

10

5

10 Events / 0.01 mm ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Signal Region <20 GeV

µ T

, 10<p µ e Post-Fit Data (top) µ Prompt (top) µ → τ (hadron decay) µ τ τ → Z Other SM processes Uncertainty 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 | [mm]

µ

|d 0.9 0.95 1 1.05 Data / Pred. 1 10

2

10

3

10

4

10

5

10

6

10 Events / 0.01 mm ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Signal Region <250 GeV

µ T

, 20<p µ e Post-Fit Data (top) µ Prompt (top) µ → τ (hadron decay) µ τ τ → Z Other SM processes Uncertainty 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 | [mm]

µ

|d 0.9 0.95 1 1.05 Data / Pred. 1 10

2

10

3

10

4

10

5

10

6

10 Events / 0.01 mm ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Signal Region <250 GeV

µ T

, 20<p µ µ Post-Fit Data (top) µ Prompt (top) µ → τ (hadron decay) µ µ µ → Z τ τ → Z Other SM processes Uncertainty

0.8 0.9 1 1.1 1.2

) ν µ → BR(W ) ν τ → BR(W ) ν e → BR(W ) ν τ → BR(W ) ν e → BR(W ) ν µ → BR(W

ATLAS Preliminary

UA1 UA2 CDF D0 LHCb LEP ATLAS PDG averages

Z.Phys. C44 (1989) 15-61

  • PLB. 280 (1992) 137-145

J.Phys.G 34 (2007) 2457-2544, PRL. 68 (1992) 3398-3402

  • PRL. 75 (1995) 1456, PRL. 84 (2000) 5710

JHEP 10 (2016) 030 Phys.Rept. 532 (2013) 119

  • EPJC. 77 (2017) 367
  • PRD. 98 (2018) 030001

ATLAS - this result

  • 1

= 13 TeV, 139 fb s Statistical Error Systematic Error Total Error

17 / 19

slide-18
SLIDE 18

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Lepton Universality in W → lν - Fit & Results

◮ A fit is performed in 3 bins in pT x 8 bins in |d0| x 2 channels (e-µ,µ-µ). ◮ Good agreement is seen in the fitted distributions. ◮ The fitted value of R(τ/µ) is found to be; . R(τ/µ) = 0.992 ± 0.013 [±0.007 (stat) ± 0.011 (syst)] ◮ The most precise measurement to date (by a factor 2) and the SM prevails.

0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 | [mm]

µ

|d 0.9 0.95 1 1.05 Data / Pred. 1 10

2

10

3

10

4

10

5

10 Events / 0.01 mm ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Signal Region <20 GeV

µ T

, 10<p µ µ Post-Fit Data (top) µ Prompt (top) µ → τ (hadron decay) µ µ µ → Z τ τ → Z Other SM processes Uncertainty 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 | [mm]

µ

|d 0.9 0.95 1 1.05 Data / Pred. 1 10

2

10

3

10

4

10

5

10 Events / 0.01 mm ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Signal Region <20 GeV

µ T

, 10<p µ e Post-Fit Data (top) µ Prompt (top) µ → τ (hadron decay) µ τ τ → Z Other SM processes Uncertainty 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 | [mm]

µ

|d 0.9 0.95 1 1.05 Data / Pred. 1 10

2

10

3

10

4

10

5

10

6

10 Events / 0.01 mm ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Signal Region <250 GeV

µ T

, 20<p µ e Post-Fit Data (top) µ Prompt (top) µ → τ (hadron decay) µ τ τ → Z Other SM processes Uncertainty 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 | [mm]

µ

|d 0.9 0.95 1 1.05 Data / Pred. 1 10

2

10

3

10

4

10

5

10

6

10 Events / 0.01 mm ATLAS Preliminary

  • 1

= 13 TeV, 139 fb s Signal Region <250 GeV

µ T

, 20<p µ µ Post-Fit Data (top) µ Prompt (top) µ → τ (hadron decay) µ µ µ → Z τ τ → Z Other SM processes Uncertainty

0.8 0.9 1 1.1 1.2

) ν µ → BR(W ) ν τ → BR(W ) ν e → BR(W ) ν τ → BR(W ) ν e → BR(W ) ν µ → BR(W

ATLAS Preliminary

UA1 UA2 CDF D0 LHCb LEP ATLAS PDG averages

Z.Phys. C44 (1989) 15-61

  • PLB. 280 (1992) 137-145

J.Phys.G 34 (2007) 2457-2544, PRL. 68 (1992) 3398-3402

  • PRL. 75 (1995) 1456, PRL. 84 (2000) 5710

JHEP 10 (2016) 030 Phys.Rept. 532 (2013) 119

  • EPJC. 77 (2017) 367
  • PRD. 98 (2018) 030001

ATLAS - this result

  • 1

= 13 TeV, 139 fb s Statistical Error Systematic Error Total Error

0.8 0.9 1 1.1 1.2

) ν µ → BR(W ) ν τ → BR(W ) ν e → BR(W ) ν τ → BR(W ) ν e → BR(W ) ν µ → BR(W

ATLAS Preliminary

UA1 UA2 CDF D0 LHCb LEP ATLAS PDG averages

Z.Phys. C44 (1989) 15-61

  • PLB. 280 (1992) 137-145

J.Phys.G 34 (2007) 2457-2544, PRL. 68 (1992) 3398-3402

  • PRL. 75 (1995) 1456, PRL. 84 (2000) 5710

JHEP 10 (2016) 030 Phys.Rept. 532 (2013) 119

  • EPJC. 77 (2017) 367
  • PRD. 98 (2018) 030001

ATLAS - this result

  • 1

= 13 TeV, 139 fb s Statistical Error Systematic Error Total Error 18 / 19

slide-19
SLIDE 19

Top Properties from ATLAS

Chris Young (CERN), on behalf of ATLAS

Conclusions

◮ ATLAS has measured many different properties of top quarks (and W boson). ◮ We have probed many different kinematic and fundamental properties in this sector. ◮ So far, the Standard Model has described the data extremely well. ◮ More results with the Run 2 dataset are in the pipeline and Run 3 (and beyond) promise even larger datasets. ◮ Many more exciting Top Physics results still to come! ◮ Coffee chat; https://zoom.us/j/97792832807?pwd=cU4waVZMNW9tWnpZcldIWHBlV2QyUT09

0.8 0.9 1 1.1 1.2

) ν µ → BR(W ) ν τ → BR(W ) ν e → BR(W ) ν τ → BR(W ) ν e → BR(W ) ν µ → BR(W

ATLAS Preliminary

UA1 UA2 CDF D0 LHCb LEP ATLAS PDG averages

Z.Phys. C44 (1989) 15-61

  • PLB. 280 (1992) 137-145

J.Phys.G 34 (2007) 2457-2544, PRL. 68 (1992) 3398-3402

  • PRL. 75 (1995) 1456, PRL. 84 (2000) 5710

JHEP 10 (2016) 030 Phys.Rept. 532 (2013) 119

  • EPJC. 77 (2017) 367
  • PRD. 98 (2018) 030001

ATLAS - this result

  • 1

= 13 TeV, 139 fb s Statistical Error Systematic Error Total Error

19 / 19