Top Quark physics with ATLAS @ LHC
Francesco Spanò Columbia University LPNHE, Paris, 24th March 2011
francesco.spano@cern.ch
Top Quark physics with ATLAS @ LHC LPNHE, Paris, 24th March 2011 - - PowerPoint PPT Presentation
Top Quark physics with ATLAS @ LHC LPNHE, Paris, 24th March 2011 Francesco Span Columbia University francesco.spano@cern.ch Outline Why top quark? The LHC is back: a top factory at work Data results: hot The ATLAS detector : a
Francesco Spanò Columbia University LPNHE, Paris, 24th March 2011
francesco.spano@cern.ch
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
mass)
2
Disclaimer: wide field, concentrate on selected topics
Data results: hot
Most recent: approved 48 hours
week.
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
3
Most massive constituent of matter
MTop~ M Gold Atom
Decay and strong production rate are tests of standard model
Various scenarios with direct/indirect
coupling to new physics: from extra dimensions to new strong forces Background to possible new physics (Higgs, SUSY)
q ¯ q t ¯ t Z
q ¯ q t ¯ t Gµν
50 100 150 200 photon/gluon neutrinos electron up down strange muon charm tau bottomW Z top
Mtop~ electroweak symmetry breaking scale
Masses of known fundamental particles
80.3 80.4 80.5 150 175 200 mH [GeV] 114 300 1000
mt [GeV] mW [GeV]
68% CL !" LEP1 and SLD LEP2 and Tevatron (prel.)
July 2010
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
4
2011
counter-rotating high intensity proton bunches colliding with 3.5 TeV/beam (ECM=7 TeV) in 27 Km tunnel
eventually: ECM=14TeV (7 TeV per beam, design value)
22nd March: Break 2010 record
peak lumi ~2.5⋅1032 cm-2 s-1
Plans: peak lumi:~0.5 to 1⋅1033cm-2 s-1 ∫Ldt between 1 and 3 fb-1
luminosity:2.1⋅1032 cm-2s-1
luminosity~50 pb-1
2010:
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
proton-proton collisions
5
~30% ~70%
top is also singly produced, but focus on dominant pair production
qq annihilation gluon fusion
@ 14 TeV : qq~10%, gg ~90%
fracesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar - 24th March 2011
6
Theory uncertainty: ~ 8 to 6% at Tevatron, 6 to 4% at LHC
LHC14
tt cross section Rate at L= 1033cm-2 s-1 √s(TeV) xsec (pb) 1.96 (pp)
7 (pp) 14 (pp) ~7 ~165 ~900
0.2Hz 0.9Hz
LHC7
for ∫Ldt =1 fb-1 @ 7TeV, expect 16*104 events Tevatron: 9.4 fb-1 on tape, expect ~ 6.6*104 events
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
l, q ν, q’ b W+
7
1.6% 4.9%
13.5% 45.7% 4.7% 29.6%
(e,mu)+jets Tau to (e,mu)+jets Fully hadronic Had tau Di-lepton (e,mu) Di-lepton (tau)
~32.4% ~67.6%
l, q ν, q’ b W+
tt had tau +jets all jets (e,μ) +jets di-lepton
ℓν qq
decays
bkgs_tt: W/Z(+jets), single top, QCD, Di-bosons
+jets
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
8
size matters
theta
EM Calorimeters Hadronic Calorimeters Inner detector
3 trigger levels for event selection
Muon spectrometer
44m 25 m
η= pseudorapidity =-ln (tan(theta/2))
phi
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
9
→
real commissioning tool: full detector at play
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
10
Data sample for first top paper~3 pb-1
Luminosity uncertainty ~ 3.4%
expect ~5700 tt events
Already collected ~ a few pb-1
fracesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar - 24th March 2011
no muon within DR< 0.4 of a jet
11
shape variables, track quality, track-cluster matching, E/p, transition radiation
scale factors to correct small data/MC mismatch
* |ηcluster|∉ [1.37,1,52] [GeV]
µ µ
m 70 75 80 85 90 95 100105 110115 Entries / 1 GeV 200 400 600 800 1000 1200 1400 1600
= 7 TeV) s Data 2010 ( µ µ ! Z
ATLAS Preliminary
L= 33 pb
"
ATLAS-CONF-2011-041
70 75 80 85 90 95 100105110115 200 400 600 800 1000 1200 1400 1600 70 75 80 85 90 95 100105110115 200 400 600 800 1000 1200 1400 1600 [GeV]
ee
m 70 75 80 85 90 95 100105110115 Entries / 1 GeV 200 400 600 800 1000 1200 1400 1600
= 7 TeV) s Data 2010 ( ee → Z QCD
L dt = 36 pb
∫
ATLAS Preliminary
ATLAS-CONF-2011-041
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
12
parton interaction
“hard stuff clusters with nearest neighbour”
Cluster significant (Ecell /
exp_noisecell)
energy deposits in calorimeters
! cos " | # |tan
0.05 ! sin " | # |tan
0.05
210
310
410
510
FCal1C
Simulated QCD di-jet
MeV
clusters→ jet with anti-kT algorithm(R=0.4)
(Cacciari,Salam, Soyez,2008)
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
13
ATLAS test beam 2004
Extensive validation of simulation in test- beam data →good collision data description
Linearity within ~2%
p[GeV] <E/P> 0.3 0.4 0.5 0.6 0.7 0.8 ATLAS Preliminary
|<1.1) ! (0.6<|
b µ Data 2010. L=866 Pythia ATLAS MC10 systematic uncertainty
p[GeV] 1 10 MC/DATA 0.9 1 1.1
single pion response for known beam energy single isolated charged hadron response vs track momentum
ATLAS colllisions 2010
Data/MC within 2% for p<10 GeV
ATLAS-CONF-2011-028
beam
/E
Comb
E 0.6 0.65 0.7 0.75 0.8 0.85
MC Data
[GeV]
beam
E 20 30 40 50 60
2
10
2
10 × 2
2
10 × 3
[%]
E Comb
∆
–4 –2 2 4 6
2%
±
ηpion =0.55
NIMA 621 (2010) 134
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
(η,pT) dependent weight from simulated “true” jet kinematics
between 2% to 8% in pT and η
and hadronization
single particle data, test beam
14
[GeV]
jet T
p
2
10
3
10 Data / MC 0.9 0.92 0.94 0.96 0.98 1 1.02 1.04 1.06 1.08 1.1 1.12 1.14 Multi-jet Track-jet
γ
γ JES uncertainty =0.6, EM+JES R
t
anti-k ATLAS Preliminary
[GeV]
jet T
p 20 30 40
2
10
2
10 × 2
3
10 Fractional JES systematic uncertainty 0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16 0.18 ATLAS Preliminary
| < 0.8, Data 2010 + Monte Carlo QCD jets η | ≤ =0.6, EM+JES, 0.3 R
t
Anti-k
ALPGEN + Herwig + Jimmy Noise Thresholds JES calibration non-closure PYTHIA Perugia2010 Single particle (calorimeter) Additional dead material Total JES uncertainty
ATLAS-CONF-2011-053 ATLAS-CONF-2011-053
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
projected in transverse plane associated with high pt
projected in transverse plane
to association to high pT object (electron, photon,tau, jet, muon)
involving jets and electrons
15
[GeV]
miss T
E 10 20 30 40 50 60 Events / 1 GeV 1 10
2
10
3
10
4
10
5
10
6
10
RefFinal
10 20 30 40 50 60 1 10
2
10
3
10
4
10
5
10
6
10
Data MC MinBias
ATLAS Preliminary
= 7 TeV s Data 2010
Ldt=0.34 nb
!
|<4.5 " | ATLAS-CONF-2010-057
[GeV]
T
E ! 50 100 150 200 250 300 Resolution [GeV]
miss y
,E
miss x
E 1 2 3 4 5 6 7 8 9 10
LCW
T
E ! Data: fit 0.49
T
E ! MC Minbias: fit 0.51
ATLAS Preliminary
= 7 TeV s Data 2010
Ldt=0.34 nb
"
|<4.5 # |
ATLAS-CONF-2010-057
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
16
for jets
matching the trigger object
channel
mass* > 25 GeV( 60GeV - ETmiss) for e
(mu) channel
pT> 25 GeV
e mu mu 3jets 4jets 3jets 4jets tt
116 194 161 273
QCD
62 22 121 51
W+jets
580 180 1100 310
Z+jets
32 18 69 25
Single t
22 11 32 15
WW,WZ,ZZ
9 3 16 4
Total Exp 830
430 1500 680
Data
781 400 1356 653
t
ν W + b
t
W – b q q'
∫Ldt =35 pb-1
ATLAS-CONF-2011-023
as
T pν T(1 − cos(φ − φν))
*=
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
17
20 40 60 80 100 120 140 160 Events / 5 GeV 100 200 300 400 500 20 40 60 80 100 120 140 160 Events / 5 GeV 100 200 300 400 500
e+2-jets
ATLAS Preliminary
L = 35 pb
∫
data t t W + jets Other Bkgd QCD uncertainty
Nloose = Nloosefake + Nloosereal
Ntight = εfake Nloosefake + εreal Nloosereal
Transverse Mass [GeV] 20 40 60 80 100 120 140 160 100 200 300 400 500 600 700 800 900 Transverse Mass [GeV] 20 40 60 80 100 120 140 160 100 200 300 400 500 600 700 800 900
+2-jets µ
ATLAS Preliminary
L = 35 pb
∫
data t t W + jets Other Bkgd QCD uncertainty ATLAS- CONF- 2011-023 ATLAS- CONF- 2011-023
μ channel: matrix method
εfake from low ETmiss ,MTW and εreal from Z→μ+μ- Looser lepton definition: control region. Assume same shape in default and control region
e channel: template method
(electron fail one/more selection criteria)
apply tight selection
events and find real fake muons from
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
18
[GeV]
jjj
m 100 200 300 400 500 600 700 Events / 20 GeV 10 20 30 40 50 60 70 80
4-jets ≥ e+
ATLAS Preliminary
L = 35 pb
∫
data t t W + jets Other Bkgd QCD uncertainty [GeV]
jjj
m 100 200 300 400 500 600 700 Events / 20 GeV 20 40 60 80 100 120 140
4-jets ≥ + µ
ATLAS Preliminary
L = 35 pb
∫
data t t W + jets Other Bkgd QCD uncertainty
ATLAS-CONF-2011-023
(WW,WZ,ZZ)
Simulated + rate set to SM prediction
Shape from simulation rate from final fit after all cuts
ATLAS-CONF-2011-023
0.5 1 1.5 100 200 300 400 500 600 700 800 900
Data t t W+jets QCD Other Bkgd
Ldt= 35 pb
∫
ATLAS Preliminary
lepton
q Events
≥
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 10 20 30 40 50 60 70 80
Data t t W+jets QCD Other Bkgd
L= 35 pb
∫
ATLAS Preliminary A) × exp(-8 Events / 0.05 francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
discriminant from distributions of
more central
symmetric,W+jets isn’t
spherical
19
ATLAS-CONF-2011-023
≥
0.5 1 1.5 2 2.5 20 40 60 80 100 120 140
Data t t W+jets QCD Other Bkgd
Ldt= 35 pb
∫
ATLAS Preliminary
lepton
η Events / 0.25
mu+>=4jets
e+>=4jets mu+>=4jets
ATLAS-CONF-2011-023
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
both channels. Fix QCD and smaller bkg, fit top and W+jets contrib.
20
ATLAS-CONF-2011-023
found as
Likelihood discriminant 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Events / 0.10 50 100 150 200 250 ATLAS Preliminary
Ldt = 35 pb
Data t t W+jets QCD Other Bkgd
e+3-jets
Likelihood discriminant 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Events / 0.10 20 40 60 80 100 120 140 160 180 200 220 ATLAS Preliminary
Ldt = 35 pb
Data t t W+jets QCD Other Bkgd
4-jets ≥ + µ
ATLAS-CONF-2011-023
σtt = Nsig
,
signal acceptance, efficiency and branching ratio from simulation + data/MC scaling factors
where
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
jet properties (scale, multiplicity) and background normalization are the dominant contributors
21
ATLAS-CONF-2011-023
Source Relative cross-section uncertainty [%] Object selection Lepton reconstruction, identification, trigger
Jet energy scale and reconstruction
Background rates and shape QCD normalisation ±3.9 QCD shape ±3.4 W+jets shape ±1.2 Other backgrounds normalisation ±0.5 Simulation Initial/final state radiation
Parton distribution functions
Parton shower and hadronisation ±3.3 Next-to-leading-order generator ±2.1 MC statistics ±1.8 Pile-up ±1.2 Total systematic uncertainty
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
same order of magnitude
22
[ pb ]
t t
σ 50 100 150 200 250 300 350 Counting
+ 48
1 5 ± 11 ± 154 (l,jet) fit
max
η ∆ 1D 24 ± 6 ± 21 ± 168 fit η 1D lepton 39 ± 7 ± 25 ± 204 Multivariate
+ 20
1 6 ± 17 ± 171
L = 35 pb
Data 2010, L+jets w/o b-tagging
Theory (approx. NNLO)
= 172.5 GeV
t
m (lumi) ± (syst) ± (stat) ATLAS Preliminary
ATLAS-CONF-2011-023
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
23
sigma_do-> different probability for jet
04'2)!"2&#"1%'(&$ *),"$+-
e d0/σd0
muons in jets, count how many are b-tagged
properties (invariant mass tracks, rate
pT dependent scale factors to correct MC
(Jet Probability)
10
1 2 3 4 5 6 7 8 9 Number of Jets
2
10
3
10
4
10
5
10
6
10
7
10
8
10
9
10 = 7 TeV s
Data 2010 Pythia Dijet MC : light jets Pythia Dijet MC : c jets Pythia Dijet MC : b jets
L ~ 15 nb ATLAS Preliminary (Jet Probability)
10
1 2 3 4 5 6 7 8 9 Number of Jets
2
10
3
10
4
10
5
10
6
10
7
10
8
10
9
10 (Jet Probability)
10
1 2 3 4 5 6 7 8 9 Number of Jets
2
10
3
10
4
10
5
10
6
10
7
10
8
10
9
10 (Jet Probability)
10
1 2 3 4 5 6 7 8 9 Number of Jets
2
10
3
10
4
10
5
10
6
10
7
10
8
10
9
10 (Jet Probability)
10
1 2 3 4 5 6 7 8 9 Number of Jets
2
10
3
10
4
10
5
10
6
10
7
10
8
10
9
10 (Jet Probability)
10
1 2 3 4 5 6 7 8 9 Number of Jets
2
10
3
10
4
10
5
10
6
10
7
10
8
10
9
10
ATLAS-CONF-2010-091
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
longitudinal activity ←top is more transverse
tagging probability←top has more b-jets
fit of discriminant to data in 3,4 and 5 jet bins
part of fit as Gaussian nuisance parameters
24
JP
w 2 4 6 8 10 12 14 Entries/0.25
10 1 10
2
10
data t t W+Jets QCD Other
L dt = 35 pb
∫
KS test: 0.25
ATLAS Preliminary
+ 4 jets µ
)
T,3p
H × exp(-4 0.2 0.4 0.6 0.8 1 Entries/0.10 20 40 60 80 100 120 140
data t t W+Jets QCD Other
L dt = 35 pb
∫
KS test: 0.11
ATLAS Preliminary
+ 4 Jets µ
ATLAS-CONF-2011-035 ATLAS-CONF-2011-035
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
methods
25
high jet multiplicity bins (3,4 and 5) ←extrapolate content of 1 and 2 jet bins before tagging
Number of b-tags 1 2 ≥ Events 100 200 300 400 500
4-jets ≥ e+
ATLAS Preliminary
L dt = 35 pb
∫
data t t W + jets Other Bkgd QCD uncertainty
ATLAS-CONF-2011-035
simulated + rate set to SM expectation
Number of b-tags 1 2 ≥ Events 100 200 300 400 500 600 700 800
4-jets ≥ + µ
ATLAS Preliminary
L dt = 35 pb
∫
data t t W + jets Other Bkgd QCD uncertainty
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
improves statistical uncertainty (enhanced background reduction)
26
[ pb ]
t t
σ 50 100 150 200 250 300 350 Counting
+ 48
1 5 ± 11 ± 154 (l,jet) fit
max
η ∆ 1D 24 ± 6 ± 21 ± 168 fit η 1D lepton 39 ± 7 ± 25 ± 204 Multivariate
+ 20
1 6 ± 17 ± 171
L = 35 pb
Data 2010, L+jets w/o b-tagging
Theory (approx. NNLO)
= 172.5 GeV
t
m (lumi) ± (syst) ± (stat) ATLAS Preliminary
[ pb ]
t t
σ 50 100 150 200 250 300 Counting
+ 34
1 6 ± 10 ± 156 Top mass standard fit
+ 20
1 6 ± 14 ± 183 Top mass profile fit
+ 18
1 5 ± 8 ± 156 Multivariate
+ 21
1 6 ± 10 ± 186
L = 35 pb
Data 2010, L+jets w/ b-tagging
Theory (approx. NNLO)
= 172.5 GeV
t
m (lumi) ± (syst) ± (stat) ATLAS Preliminary
as statistics; already dominant in b-tagging case
ATLAS-CONF-2011-035 ATLAS-CONF-2011-023
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
27
exactly two opposite sign high pT central leptons (ee, eμ, μμ) and ≥ 2 central high pT jet
activity
t
ν l+ W + b
t
W – b q q'
l-
ν
Z/γ*+jets QCD, Di-bosons single lepton
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
samples enriched with real and “fake” leptons
be in signal region
signal and control samples
28
ee µµ eµ Z/γ∗+jets (DD) 1.2+0.5
−0.6
3.4+1.9
−1.4
0.4+0.4
−0.3
1.2+0.7
−0.6
3.2+1.6
−1.3
Non-Z leptons (DD) 0.8 ± 0.8 0.5 ± 0.6 3.0 ± 2.6 Single top (MC) 0.7 ± 0.1 1.3 ± 0.2 2.5 ± 0.4 Dibosons (MC) 0.5 ± 0.1 0.9 ± 0.2 2.1+0.5
−0.3
Total (non t¯ t) 3.5 ± 1.1 7.3+1.8
−1.5
10.8 ± 3.4 t¯ t (MC) 11.5 ± 1.3 20.1 ± 1.7 47.4 ± 4.0 Total expected events 15.0 ± 1.7 27.4 ± 2.4 58.2 ± 5.2 Observed events 16 31 58 [GeV]
miss T
E 50 100 150 200 Events / 5 GeV
10
10 1 10
2
10
3
10
4
10
5
10 [GeV]
miss T
E 50 100 150 200 Events / 5 GeV
10
10 1 10
2
10
3
10
4
10
5
10 [GeV]
miss T
E 50 100 150 200 Events / 5 GeV
10
10 1 10
2
10
3
10
4
10
5
10 data t t single top DY + jets diboson fake leptons uncertainty
control region µ µ
ATLAS Preliminary
L = 35 pb
∫
Events 10 Events 10 Events 10
ATLAS- CONF-2011- 027
(SigReg)/MCZ/γ (ConReg) ]
invariant mass [GeV]
+
e 20 40 60 80 100 120 140 160 180 Events / 10 GeV 1 10
2
10
3
10
4
10 invariant mass [GeV]
+
e 20 40 60 80 100 120 140 160 180 Events / 10 GeV 1 10
2
10
3
10
4
10 invariant mass [GeV]
+
e 20 40 60 80 100 120 140 160 180 Events / 10 GeV 1 10
2
10
3
10
4
10 data t t single top DY + jets diboson fake leptons uncertainty
control region ee
ATLAS Preliminary
L = 35 pb
∫
ATLAS- CONF-2011- 027
in Z window for low ETmiss
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
including systematics as nuisance parameters
29
Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10 Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10 Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10 data t t single top DY + jets diboson fake leptons uncertainty
ee
ATLAS Preliminary
L = 35 pb
∫
Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10 Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10 Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10 data t t single top DY + jets diboson fake leptons uncertainty
µ µ
ATLAS Preliminary
L = 35 pb
∫
Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10
7
10 Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10
7
10 Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10
7
10 data t t single top DY + jets diboson fake leptons uncertainty
µ e
ATLAS Preliminary
L = 35 pb
∫
ATLAS-CONF-2011-027
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
30
[ pb ]
t t
σ 50 100 150 200 250 300 b-tagging fit 22 ± 6 ± 22 ± 176 / Z t t 20 ± 22 ± 178 inclusive 14 ± 5 ± 22 ± 171 Counting w/ b-tagging
+ 21
1
+ 7
1 22 ± 171 Counting
+ 18
1
+ 8
1 22 ± 173
L = 35 pb
Data 2010, Dilepton
Theory (approx. NNLO)
= 172.5 GeV
t
m (lumi) ± (syst) ± (stat) ATLAS Preliminary
ATLAS-CONF-2011-027
[ pb ]
t t
! 50 100 150 200 250 300 Dilepton w/ b-tagging
+ 21
1
+ 7
1 22 ± 171 L+jets w/o b-tagging
+ 20
1 6 ± 17 ± 171 Combination 15 ± 6 ± 9 ± 180 Dilepton w/o b-tagging
+ 18
1
+ 8
1 22 ± 173 L+jets w/ b-tagging 20 ± 6 ± 10 ± 186
L = 35 pb
"
Data 2010,
Theory (approx. NNLO)
= 172.5 GeV
t
m (lumi) ± (syst) ± (stat) ATLAS Preliminary francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
10%: comparable to theory
31
[TeV] s 1 2 3 4 5 6 7 8 [pb]
t t
! 1 10
2
10
ATLAS Preliminary )
(35 pb CMS )
(36 pb CDF D0
NLO QCD (pp)
) p NLO QCD (p ) p
6.5 7 7.5 100 150 200 250 300
dominated by systematics
35 pb-1
6.5 7 7.5 100 150 200 250 300 6.5 7 7.5 100 150 200 250 300
3 pb-1
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
32
[GeV]
reco W
m 40 60 80 100 120 140 Events / 6 GeV 10 20 30 40 50 60 70 40 60 80 100 120 140 10 20 30 40 50 60 70
= 7 TeV data s =172.5 GeV
top, m t t =172.5 GeV
tops-top, m Z+jets W+jets WW,ZZ,WZ QCD
Preliminary ATLAS
35 pb
32
R 1 2 3 4 5 6 7 8 Events / 0.3 5 10 15 20 25 30 35 40
32
R 1 2 3 4 5 6 7 8 Events / 0.3 5 10 15 20 25 30 35 40
=7 TeV data s Best Fit background + background t Best Fit t 5.0 GeV ± = 166.7
top
m
ATLAS Preliminary ATLAS
L = 35 pb
∫
[GeV]
topm
160 165 170 175
1 2
mu channel
32
R 1 1.5 2 2.5 3 3.5 4 4.5 5 Normalized Events / 0.1 0.02 0.04 0.06 0.08 0.1 0.12 0.14
32
R 1 1.5 2 2.5 3 3.5 4 4.5 5 Normalized Events / 0.1 0.02 0.04 0.06 0.08 0.1 0.12 0.14
32
R 1 1.5 2 2.5 3 3.5 4 4.5 5 Normalized Events / 0.1 0.02 0.04 0.06 0.08 0.1 0.12 0.14
32
R 1 1.5 2 2.5 3 3.5 4 4.5 5 Normalized Events / 0.1 0.02 0.04 0.06 0.08 0.1 0.12 0.14
32
R 1 1.5 2 2.5 3 3.5 4 4.5 5 Normalized Events / 0.1 0.02 0.04 0.06 0.08 0.1 0.12 0.14
= 160 GeV
top
m = 170 GeV
top
m = 180 GeV
top
m = 190 GeV
top
m
sig
P
ATLAS Preliminary ATLAS Simulation = 7 TeV s
e channel
ATLAS- CONF-2011-033 ATLAS-CONF-2011-033 ATLAS-CONF-2011-033
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
final state radiation
33
[GeV]
top
m 140 150 160 170 180 190 200 13
0.0 ± 0.0 ± 0.0
Tevatron July 2010
0.9 ± 0.6 ± 173.3
1d TMT, KLF, comb
7.5 ± 2.7 ± 174.8
+jets µ 1d TMT, KLF,
7.5 ± 3.5 ± 172.0
1d TMT, KLF, e+jets
7.5 ± 4.3 ± 179.0
2d TMT, comb
4.4 ± 4.6 ± 166.1
+jets µ 2d TMT,
4.6 ± 6.7 ± 163.5
2d TMT, e+jets
4.3 ± 6.2 ± 168.3
), comb
32
default (1d TMT, R
4.9 ± 4.0 ± 169.3
+jets µ ),
32
default (1d TMT, R
5.0 ± 5.0 ± 166.7
), e+jets
32
default (1d TMT, R
4.8 ± 6.7 ± 173.8
ATLAS Preliminary ATLAS
= 35 pb
int
(syst.) ± (stat.) ±
[GeV]
top reco
m 100 200 300 400 500 600 700 Events / 25 GeV 5 10 15 20 25 30 35 40 45 [GeV]
top reco
m 100 200 300 400 500 600 700 Events / 25 GeV 5 10 15 20 25 30 35 40 45
=7 TeV data s =172.5 GeV
top, m t t =172.5 GeV
tops-top, m Z+jets W+jets WW,ZZ,WZ QCD
L = 35 pb
∫
Tagged e + jets Preliminary ATLAS
top peak from kinematic fitter
ATLAS-CONF-2011-033 ATLAS-CONF-2011-033
Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
34
@ Tevatron: Z’mass < 850 GeV @95%CL @LHC: CMS @ MoriondEWK11 showed upper limits on Z’ xsec
Example : resonances decaying to top
q ¯ q t ¯ t Z
Status for Z’
arxiv:0712.2325
Mtt [GeV] 500 1000 1500 2000 2500 Fraction of events 0.2 0.4 0.6 0.8 1
ATLAS Preliminary
Simulation, parton level
No parton merged 2 partons merged 3 partons merged
(a) topology
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
35 [GeV] t M_t 200 400 600 800 1000 1200 1400 1600 (1/30.0GeV) t 1/N dN/dM t 0.0005 0.001 0.0015 0 002 0.0025 0.003 0.0035 0 004
True di-top mass Reconstructed di-top mass Full event fit
(a) ATLAS
boosted “top jet”→ new reco to separate QCD, tt, possible new physics.
to choose jets (pT order,χ2)
MW, Mtop
advanced state. Expect results soon.
ECM =10 TeV,100 pb-1
Simulated tt
Probability to find partons within DR=0.8
ATLAS-PHYS-PUB-2010-008
hep-ex:0901.0512
pTtop~600 GeV
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
substructure and shapes
jet mass and scale for large cones, splitting scales.
expected reach resonance masses well beyond 1 TeV
(ATL_PHYS_PUB_2010_008) →exciting time
for searches!
36
) [GeV] t mass(t 500 1000 1500 2000 2500 3000 /60 GeV
events/200 pb 5 10 15 20 25 30 35 40 45
1000 2000 1 10 t SM t W+jets t
QCD
ATLAS Preliminary Simulation
= 10 TeV, 200 pb s
(b) mono-jet approach
Mono-jet reco
Track jet mass [GeV] Calorimeter jet mass [GeV] 50 100 150 200 250 300 350 Track jet mass [GeV] 20 40 60 80 100 120 Data / MC
0.8 0.9 1.0 1.1 1.2
ATLAS Preliminary
|<1.0
anti-k > 30 GeV
T> 250 GeV, p
T,leadp MC QCD Jets = 1)
PV(N
Data Ldt = 13.8 pb
Data Ldt = 13.8 pb Data (|JVF| > 0.99)
[GeV] Model mass m 1000 1200 1400 1600 1800 2000 ) limit [pb] t t ! BR (X " # 1 2 3 4 5 6 7 8 9
KK gluon, mono-jet approach No systematics (FC) Systematics included (FC) 1 STD range (hep-ph/0701166) KK gATLAS
= 10 TeV, 200 pb s Preliminary, simulation
ATLAS-PHYS-PUB-2010-008
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
at the LHC.
channel are in good agreement with standard model expectations. Systematics dominated: 180±18 pb. Improvements will need to focus on reduction of systematics uncertainties.
prospects for new physics searches with top, for instance top resonances
37
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
39
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
Session, 23rd March 2011
40
https://indico.cern.ch/conferenceDisplay.py?confId=130457
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
Session, 23rd March 2011
41
https://indico.cern.ch/conferenceDisplay.py?confId=130457
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
42
$%&'(#)*+*(+,-#.*(/0,1,2
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
vertex, electrons, muons, jets and missing energy
43
Z
phi
Top is a real commissiong tool: full detector at play
eta
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
44
b-tagging track, particle identifcation, pt measurement
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
45
electron and jets reconstruction Missing transverse energy
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
46
!"#$%&'()%*+%&,-./%(-0&1 2-3$&1 4"(&5678&9::; <-+$#&=$>.-7&?$#*@.$"*-7 ! AB&C0$7D
!"#!$%&'( )!"!*+ !"#,'--./#)!",+ 0'%-1$2&#!$%&'( )0!*+ 31-4'-%# )3*56+ 72/.#!89.$%.%#,'--./ 72/.#,'--./ !"#$%&'()*(+"&%#$",-.(&%/01$23%-.( 4#"13,"#$&'.(5$**%#%1&(6%#*)#+"1/%- ↓ 7%%5(/)0%#%1&(8$%9:
01%#!*234 5
6 7'**-(%801795%:η:%;%<=> 6 0?@&'A 8010&95% <=B;:η:;C=D
E'@*)? &'()*+,-.-*F
6 7'**-(%8"+(-9%$G+?.+(=2 $.--(5%:η:;<=H 6 0?@2&'A%8E0&95%#!*2&I% <=>;:η:;C=D
J)*K'*@%&'()*+,-.-*%
C=D%;:η:;%>=L
6 JG'(<5%#!*2&I 6 JG'(DMC5%#!*2N
F Spanò, Local Hadron calibration, Atlas Physics Workshop Rome 2005
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
47
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
48
Back
Front Presampler
Cryostat
Signal definition (Clusters) Invisible energy Out of cluster Dead material Leakage LAr EM Cal Tile Had Cal Incoming hadron Weight 7 layers Correct Had Calib
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
suppress noise
mass closest to “true” stable particle jets
49 !"#$%&'() $*+(#) &',)$(#) !"#$%&'() $*+(#) &',)$(#) !"#$%&'() $*+(#) &',)$(#)
0.1 ! "#" ! 2.3 4.1 ! "#" ! 5.2 0- 6(7 0-- 6(7 0--- 6(7 ! !" !"" ! !" !"" ! !" !"" ! # $ % &'()*+( ,-./() 01 20,3454-(,43 6() 7(4 '*8 9 $ :8(9;
0- %<=><? @A <=><? @A <=><? @A
!"#$%&'( )($ $*+(# )($ &',-$(# )($ !"#$%&'( )($ $*+(# )($ &',-$(# )($ !"#$%&'( )($ $*+(# )($ &',-$(# )($
! " .// 0(1
#$% &
! " 2// 0(1
#$% &
! " . 3(1
#$% &
! !"# $ $"# % %"# &
'*4 5#5! '(6)'()6
./ &
! %! *! +! ,! $!! %! *! +! ,! $!! %! *! +! ,! $!!
*+,
7897: 0;
di-jet simulated events, anti-kT R=0.6
hep-ex:0901.0512 hep-ex:0901.0512
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
for ) Zto ee and Z ti mumu NLO factor of 125
50
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
parameter significance for each track in jet to resolution function to find track prob. to originate
51
Ptrki =
−|di
0/%i d0|
−&
R(x)dx. n can be determined from experimental data
d
S
10 20 30 40 Number of tracks 1 10
2
10
3
10
4
10
5
10
6
10
7
10
8
10
9
10
L ~ 15 nb = 7 TeV s
Data 2010 Pythia Dijet MC : light jets Pythia Dijet MC : c jets Pythia Dijet MC : b jets
ATLAS Preliminary
3
10
4
10
5
10
6
10
7
10
Pjet = P0
N−1
!
k=0
(−lnP0)k k! ,
The region around Sd0 0 is zoomed in in the inset.
dS
10 20 30 40
10
10
10
10
10
10
10 1
Data
ATLAS Preliminary
dS
10 20 30 40
10
10
10
10
10
10
10 1
Monte CarloATLAS Preliminary
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
52
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
53
Emiss
x(y) = Emiss,calo x(y)
+Emiss,cryo
x(y)
+Emiss,muon
x(y)
above equation, referred to as the calorimeter, cryo
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
54
Emiss
x(y) = Emiss,calo x(y)
+Emiss,cryo
x(y)
+Emiss,muon
x(y)
above equation, referred to as the calorimeter, cryo
Emiss,calo,calib
x(y)
= Emiss,e
x(y)
+Emiss,!
x(y)
+Emiss,"
x(y)
+Emiss,jets
x(y)
+Emiss,calo,µ
x(y)
+Emiss,CellOut
x(y)
ere each term is calculated from the negative sum of calibrated cell energies inside the corre
Emiss,µ
x(y)
= −
!
selected muons
Eµ
x(y)
Emiss,cryo
x(y)
= −!
jets
Ejet,cryo
x(y) Ejet,cryo
x
= wcryo
EM3 ×Ejet HAD1
cos"jet cosh!jet Ejet,cryo
y
= wcryo
EM3 ×Ejet HAD1
sin"jet cosh!jet ration factor, determined together with the cell sign
isolated muons non-isolated muons
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
bin multiplicity are such that
55
W≥4-jet
tagged = W≥4-jet pre-tag · f ≥4-jet tagged.
e W jets event count in the pre-ta
f ≥4-jet
tagged = f 2-jet tagged · f corr 2→≥4,
the W jets tag fraction in the
W≥4-jet
pre-tag = W2-jet pre-tag · ∞
(W2-jet
pre-tag/W1-jet pre-tag)n,
extrapolate to a sample with four or more jets
Wn+1-jets/Wn-jets~constant (Berends
,Giele)
Wn-jets/W2-jets=Wn-jets/Wn-1je * (Wn-jets/Wn-1jet....
Estimate pre-tagged amount of W+jets in 4-jet bin then correct it to tagged sample
Measured by subtracting simulated nonW bkg in 1,2 jet bin, before b-tagging
good agreement data/MC in control region Subtract MC in content of 2jet bin bef and after tagging. Take ratio (only in mu, less QCD)
from simulation
as f corr
2→≥4 = f ≥4-jet tagged/ f 2-jet
ined to be:
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
properties (scale, multiplicity) and heavy flavour contents are the dominant contributors
and PDF uncertainty relative importance is reduced w.r.t to no b- tagging
56
Statistical Error (%) +5.3
Object selection (%) Jet energy scale +3.8
Jet reconstruction efficiency +4.2
Jet energy resolution +0.8
Electron scale factor +1.2
Muon scale factor +0.5
Electron smearing +0.3
Muon smearing +0.6
Background modeling (%) Wjets HF content +7.2
Wjets shape +1.5
QCD shape +1.0
t¯ t signal modeling (%) ISR/FSR +4.0
NLO generator +0.5
Hadronisation +0.0
PDF +1.7
Others (%) b-tagging calibration +7.5
Simulation of pile-up +1.5
Templates statistics +1.6
Total Systematic (%) +11.5
ATLAS-COM-CONF-2011-028
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
57
nom tt
σ /
tt
σ injected 0.5 0.6 0.7 0.8 0.9 1 1.1 1.2 1.3 1.4 1.5
nom tt
σ /
tt
σ fitted 0.5 0.6 0.7 0.8 0.9 1 1.1 1.2 1.3 1.4 1.5 0.0047 ± p0 = 0.0055 0.0047 ± p1 = 0.9987 ATLAS Preliminary Simulation
tt
σ δ ) /
nom tt
σ
tt
σ (
1 2 3 4 5 Pseudo experiments 20 40 60 80 100 120 140 160 0.032 ± Mean = 0.065 0.025 ± = 0.979 σ ATLAS Preliminary Simulation
expected stat uncertainty is 9.7%
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
58
120 140 160 180 200 120 140 160 180 200
Simulation Fit χ2/ndof: 3.0 / 7 Slope: 0.99 ± 0.01 Offset: 1.14 ± 1.07
Fitted σtt [pb] Input σtt [pb]
ATLAS Preliminary
120 140 160 180 200
Pull
1
Input σtt [pb]
ATLAS Preliminary
Simulation
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
59
lepton
quality for jets
high pT central leptons (ee, e,mumu) matching the trigger
pT> 20 GeV
decays and vector mesons
candidates mu pairs with large
back in r/phi
muon and electron tracks
transverse momenta
Common ee, mumu e,mu
Cuts optimized for significance of signal over bkg
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
samples relaxing
terms of unknown (real, fake) and estimated probabilities r (f): for real (fake) leptons passing loose also to pass tight cuts
60
NTT NTL NLT NLL = rr r f fr f f r(1 − r) r(1 − f) f(1 − r) f(1 − f) (1 − r)r (1 − r) f (1 − f)r (1 − f) f (1 − r)(1 − r) (1 − r)(1 − f) (1 − f)(1 − r) (1 − f)(1 − f) NRR NRF NFR NFF
Measure r in Z →ll Measure f in QCD enriched sample: single loose lepton, low ETmiss
(W+jets subtracted using simulation)
Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10
7
10
8
10
9
10
10
10 Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10
7
10
8
10
9
10
10
10 Number of jets 1 2 3 4 ≥ Events
10 1 10
2
10
3
10
4
10
5
10
6
10
7
10
8
10
9
10
10
10 data t t single top DY + jets diboson fake leptons uncertainty
control region ee
ATLAS Preliminary
L = 35 pb
∫
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
measured Z decay rate
WW and Z tauta
transverse energy cuts
tagged jets to extract tt cross section and b-tagging efficiency
61
Number of b-tagged jets 1 2 3 1 2 3 1 2 3 Events 5 10 15 20 25 30 35 40 45 Number of b-tagged jets 1 2 3 1 2 3 1 2 3 Events 5 10 15 20 25 30 35 40 45
combined
ATLAS
L = 35 pb
∫
ee µ µ µ e
Preliminary data tag counting fit S+B bkg Number of b-tagged jets 1 2 3 1 2 3 1 2 3 Events 5 10 15 20 25 30 35 40 45
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
also have large transverse mass
energy, but small transverse mass
mass discriminates the two
62
Transv Mass Transv Missing energy
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
63
σ(t¯ t) = Nsig L × = Nobs − Nbkg L ×
weighted sum of templates (in 3, 4, 5 jet bin) in two ways
parameters in fit
parameters to assess systematics
1000
[GeV]
jjj
m
200 400 600 800 1000
Events / (25 GeV)
10 20 30 40 50
+jets] µ [ Data Model Background
4 jets / 1 b-tag ≥
L dt = 35 pb
ATLAS Preliminary
Require >= 1 b-tagged jet
ATLAS-CONF-2011-035
[e+jets]
francesco.spano@cern.ch Top Quark with ATLAS @ LHC LPHNE Seminar -24th March 2011
64
Uncertainty [GeV] Electron channel Muon channel Statistical uncertainty 6.7 5.0 Method calibration 0.7 0.5 Signal MC generator(P vs. MC@NLO) 0.7 0.6 Hadronization P (P vs. H) 1.0 0.5 Pileup 0.6 0.8 ISR and FSR (signal only) 2.2 2.6 Proton PDF 0.6 0.5 W/Z+jets background normalization (±100%) 1.3 1.7 W/Z+jets background shape 0.6 1.0 QCD background normalization (±100%) 0.8 0.7 QCD background shape 0.6 0.5 Jet energy scale (±1σ) plus 5% for close by jets 2.3 1.9 b-jet energy scale (±2.5%) 2.5 2.5 b-tagging efficiency and mistag rate 0.6 0.5 Jet energy resolution 0.6 1.1 Jet reconstruction efficiency (±2%) 0.6 0.5 Total systematic uncertainty 4.8 5.0