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A measurement of σ(ttbar) & a
search for V+A structure in the
tWb vertex in CDF
Susana Cabrera
IFIC(CSIC-UV)
XXXIV International Meeting on
Fundamental Physics
FROM HERA AND THE TEVATRON TO THE LHC
April 2-7; El Escorial, Madrid,SPAIN
XXXIV IMFP 2006, April 6th
Susana Cabrera
Page 1
Top pair production at the Tevatron
Cacciari et al.
JHEP 0404:068 (2004)
Kidonakis & Vogt
PRD 68 114014 (2003)
Very rare process
One top pair each
1010 inelastic collisions
at s = 1.96 TeV
At √s=1.96 TeV:
85% qq
15% gg
σ = 6.7 pb (MTOP=175GeV)
At √s=14 TeV:
10% qq
90% gg
σ = 833 ± 100 pb
XXXIV IMFP 2006, April 6th
High Pt lepton triggers
are very important
Susana Cabrera
Page 2
Top pair decay: signatures at CDF.
1st) Test the QCD calculations
of top pair production:
By measuring top pair rate.
q’,

q,
l+
•t →Wb ~ 100% (Standard Model)
•Main “usable” event topologies
•tt  llbb di-lepton
5% e+
•tt  lqqbb lepton+jets 30% e+
•tt  qqqqbb all hadronic 45%
W
t
+
p
b
p
b
t
W
-
q, l-
q’,

2nd) Test top decay:
Measuring W helicity: look for V+A structure.
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Page 3
The Top dilepton channel event selection
tt  (W  b)(W b )  (  b)(  b )   e, ,
Two High Pt leptons:
e(Et>20GeV) or µ (Pt>20GeV)
b
q
3 dilepton channels: ee,eµ,µµ
t
e,µ
W

Reject cosmics, conversions,trileptons

Veto Z´s:
W
e,µ
q
t
ee & µµ 76< Mee,µµ< 106 GeV
jetsig  E T /  E T  8  E T
b


  (ET jet  E T / E )
MET>25 GeV:
“L-cut”
E
 T  50 GeV if min ( E
 T , (l , jet))  20o
NJETS>=2
(ET>15 GeV & |η|<2.5)
HT>200 GeV HT  {E T , ´s, jets}CORR
Opposite sign leptons.
XXXIV IMFP 2006, April 6th
Data used here
Central electron and muon triggers
and plug electron plus MET
Susana Cabrera
Page 4
ttbar Acceptance
•1M ttbar PYTHIA 6.1 MC
•MTOP=175GeV
•|zvtx|<60cm (95.5% CDF luminous region)
b
q
t
q
t
e,µ
W


W
e,µ
b
•Araw=0.873 +- 0.012% (ee : µµ: eµ) (22%:25%:53%)
Cl1l2
DT
DT
EidDT1 EedDT2 Erec
E
2
 E z 0  ( Etrg1  Etrg 2  Etrg1 Etrg 2 )  ( MC MC )( MC1 rec
)
MC
Eid1 Eid 2 Erec1 Erec 2
i
ACORR   ARAW
 C1 2
i
•Acorr=0.732 +- 0.012 %
•(ee : µµ: eµ)
• (↓90.1%:↓78.1%:↓83.7%)
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Page 5
The backgrounds: WW,WZ,Z→ττ

q
e,µ

Z/*
σZττ=333 +- 33 pb

q

e,µ
e,µ
q

W

q
e,µ
W
q
Z
q(')
W
qq´→γ*/Z→ττ +(≥2 p)
l
l
q,l
qq´→WW→lνlν+(≥2p)
σWW=12.4 +- 0.8 pb
qq´→WZ→(qq´)(ll´)
qq´→WZ→(lν)(l´l´´)
σwz=3.65 +- 0.26 pb
q('),ν
•Almost 100% MC driven:
•Pythia (LO) for raw
acceptances
•Latest NLO
predictions
•MC shortcomings: jet
multiplicity from extra
QCD radiation
•NJET scale factors
measured from Z
boson data
N
Z DATA
 2 jets
Z MC
 2 jets
N
N
PRED
BKG
  C1 2
i
MC ALL CUTS

N
/ MC
BKG

 SFDATA

2 jets
 N MC TOT
BKG

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
THEO
   BKG
Li

Page 6
Instrumental backgrounds: “Fakes” and DY
q
Origin: manly W(lv)+>=3 jets, others Wbb,Wcc,Wc, QCD
•
•
Jets faking high Pt electrons: η, π0, π+, πTracks faking high Pt muons: Semileptonic B decays, punch-through
•
W
q
Methodology:
•
e,μ

Fake lepton rates measured in high statistics jet triggered data Et (20-100) GeV
• FR(Pt)= Nl/Nd : l: electron or muon, d: fakeable object:
• Jet with Ehad/Eem<0.125
• High Pt isolated track with E/P<1
Applied to “fakeable” events l1+d2+MET+>=2 jets in W+jets data.
PREDICTED
N FAKE
BKG   FRi ( PT j )  N fakeable
i, j
Drell-Yan qq´→γ*/Z→ee,µµ +(≥2 p)
Methodology:
Use DATA in the high MET region inside the Z peak (76 <Mll<106)
Use DY Pythia MC
•Correct non-DY sources of dileptons
•To predict the number of events outside the Z mass window
•To distribute them among different jet multiplicity bins: 0,1,>=2
j
DATA
Bkg
N INj  f Zveto
( N Zveto
 N Zveto
)
XXXIV IMFP 2006, April 6th
j
j
N DY
 N OUT
 N INj
Susana Cabrera
q

q
e,µ
e,μ
j
j
out / in
DATA
Bkg
N OUT
 f MET
 RMET
( N MET
 N MET
)
Page 7
CONTROL REGIONS
NJETS=0,1 CONTROL REGIONS
2 high Pt leptons, Z veto, high Met
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SIGNAL
REGION:
NJETS>=2
HT>200GeV
OS leptons
Page 8
SUMMARY 750 pb-1
N OBS  N BKG
 tt 
 Ai  Li
i
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σtt in 750 pb-1
 tt  8.3  1.5stat  1.0 syst  0.5lumi pb
 ttTHEO  6.7 pb M.Cacciari,et al. JHEP 404,68 (2004)
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KINEMATICS (I)
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KINEMATICS (II)
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Top dilepton candidate with one b-tag
•Nrun=193051, Nevt=1108405
•1st e: Pt=114.1 GeV Eta=-0.4
•2nd e: Pt=60.3 GeV Eta=0.4
•1st jet: Et=40.3 GeV Eta=0.0
•2nd jet: Et=40.0 GeV Eta=1.1
•MET Et=55.0 GeV Eta=1.1
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From Lepton+Jets WG: 695pb-1
SIGNATURE
1 Isolated lepton
PT>20GeV/c
Met>20GeV
>=3 jets with Et>15GeV/c
CDF
BACKGROUNDS
W+jets with HF (gbb, cc)
Mistags
Non W background
>=1 b-tag
HT >200 GeV
>=2 b-tags
2 b tags
33
46
7.2+-1.3 1.9+-0.5
156
158
53.0+-6.3
17.2+-1.9
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CDF Summary XS (750 pb-1)
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
t W b
Is it really SM Top ?
SM f V+A=0 f-=30%
non SMf V+A = 1 f-=0
 (1  cos * ) 2
f0=70%
f0=70%
f+=0%
f+=30%
 (1  cos 2   )
p  pb  E  Eb
2 M lb2
cos 
 2
1


2
| p |  | pb |
mtop  M W
*
XXXIV IMFP 2006, April 6th
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Page 16
Mlb
M 2b 


1
2
M TOP
 M W2 1  cos *
2

SAMPLES:
L+jets single-btagged: 1D template, one pairing, one Mlb value
L+jets double-btagged: 2D template: 2 lepton-bjet pairing
2 entries per event: Mlb(1) vs Mlb(2)
Dileptons
Idem L+jets
Hipothesis: leading jets are b-jets
XXXIV IMFP 2006, April 6th
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Page 17
Binned Log likelihood method
SM: f
Free parameters
Dilepton Templates:
ttbar V+A,V-A
(MC, Alpgen+Pythia)
DY/WW/WZ
MC: (Alpgen+2p)
FAKES
fakeable events in
W+jets data X FR(PT)
XXXIV IMFP 2006, April 6th
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Page 18
Pseudo-experiments: test robustness
1.
2.
3.
4.
Hypothesis: f V+A= f TRUE [0,1]
Fluctuate N expected with gaussians:
1. N PE,EXP BKGR = σ EXP BKGR L
2. N PE,EXP V+A= ε V+A σ TTBAR f TRUE
3. N PE,EXP V+A= ε V+A σ TTBAR f TRUE
4. Compute expected fractions of BKGR, and signal V+A,V-A
Fill ramdomly BKGR,V+A,V-A pseudo-templates with NPE,BKGR, N PE,V+A,
NPE,V-A PE events from BKGR,V+A,V-A templates.
Perform fit: input f TRUE free parameters f V+A σttbar σBKGR, output f V+A FITTED
XXXIV IMFP 2006, April 6th
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Page 19
Confidence Level
• 1000 PE´s with a fixed true
value of fV+A
• For each pseudo-experiment:
• Get 95% CL by
‘scanning’ the likelihood
function along the fV+A
axis.
SYSTEMATICS NOT
YET INCLUDED
• After all 1000 PE’s at
different f V+A true:
•
a distribution of 95% CL’s.
• 95% CL contours: 1K PE
scanning f TRUE in [0,1]
XXXIV IMFP 2006, April 6th
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CONCLUSIONS & PROSPECTS
•11 years after the discovery and still elucidating..
•We have measured the ttbar production cross section in the dilepton
channel with 750 pb-1
CDF
 tt  8.3  1.5stat  1.0 syst  0.5lumi pb
•This result is combined with other results from l+jets channel
achieving a precision of 12%, close to the theoretical error of the
current QCD calculations of the top pair production.
•A technique to search for V+A top decay vertex in both dilepton and
lepton plus jets top samples has been extensively tested using
pseudoexperiment.
•Prospects:
•Including systematics in the 95% CL.
•Then we will open the box and measured fV+A with CDF data.
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BACKUP SLIDES
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CDF
From Run I:
•Solenoid
•Central muon system
•Central calorimeter
New For Run II:
•Front-end DAQ
•Trigger:Track (L1) and
Displaced Track (L2)
•Silicon Tracker (8 Layers)
(  2.0)
•Central Outer Tracker
(  1.0)
•Plug Calorimeters
(1.0    3.6)
•Extended Muon Coverage
(  1.5, gaps filled in)
XXXIV IMFP 2006, April 6th
||=
1. Run II Detector
CDF
||=2.
PT
PT2
 0.15% (GeV / c ) 1
Susana Cabrera
Page 23
11 years after the top quark discovery
●
●
1995: Top quark discovered by CDF and D0
–
Not a surprise: SM quark sector completed
–
But top mass was surprisingly high.
2006 (still elucidating!):
–
Single top remains undiscovered.
–
Precision measurements:
●
Pair production cross-sections:
–
Now CDF 12%
5 orders of
magnitude
Mtop (Moriond 2006)= 172.5 ± 2.3 GeV
Top properties (besides the top mass) studies
with almost 1 fb-1 .
● Is it really a Standard Model Top ?
●
–
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Page 24
• Delivered: 1.2fb-1
• Accelerator doing
very well:
– Record peak inst.
luminosity:
• 1.79x1032/cm2s
(11/10/2005)
– If no further
improvements:
Where do I get this?
Data used here
• 4fb-1 in 2009
– Electron cooling on
track
• Could get 8fb-1 in 2009!
• Detectors doing well:
– Upgrades finishing up
to deal with luminosity
increase
XXXIV
IMFP 2006,coming
April 6th in
Susana Cabrera
Page 25
Acceptance versus Top Mass
Raw acceptance changes by +0.055% per
Δ(MTOP) = 1 GeV or Δ(Acc) = -0.016%
XXXIV IMFP 2006, April 6th
Susana Cabrera
Page 26
XS versus TOP MASS
At a top quark mass of 172.0 +- 2.7 GeV/c2
(CDF 750 pb-1, March 2006)
The combined cross section is 7.53+-0.87 pb
XXXIV IMFP 2006, April 6th
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Page 27
Lepton+Jets Channel: b Tagging
CDF
2 b tags
HT>200GeV
XXXIV IMFP 2006, April 6th
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Page 28
Top dilepton candidate
Nrun=193031 Nevt=7271850
XXXIV IMFP 2006, April 6th
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Page 29
From Tevatron to the LHC
XXXIV IMFP 2006, April 6th
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Page 30
e & μ in
CDF
Central e: ||<1.2
Et>20-25 GeV
EM cluster + Drift chamber
track,Pt>10 GeV
Loose :
e &  at CDF Run II
Tight  :
Plug e: 1.2<||<2.0-2.8
EM cluster (+ Silicon track)
High Pt isolated track
pointing to a gap in the
- coverage ||<1.2
Drift
chamber
pointing to a  -stub
||<1.
 measured with Z 
measured with Zee
Trigger : 88%-95%
Trigger : 100%, Et>30 GeV
ID  : 85%-90%
ID  : >[80-94]%
Track quality
|d0|<0.2,0.02 cm
Ehad/Eem<0.055,Shower profiles,
MIP: Eeom<2 GeV
Track quality,showermax matching
Ehad<6 GeV
•Veto cosmics using timing information and track information.
E
•Veto  from jets (mostly b) using calorimeter-Isolation
•Veto e coming from photon conversions using track information.
XXXIV IMFP 2006, April 6th
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THE OUTLINE
• Top pair production.
•The Dilepton channel.
•Event selection.
•Signal acceptance.
•Background estimates.
•Main Systematics & XS measurement.
•The Lepton plus jets channel results
•Latest XS results from CDF.
• Top properties.
•Measurement of f V+A in the tWb vertex.
•Mlb observable.
•Likelyhood technique.
•Pseudoexperiments and expected limit.
• Conclusions & Prospects.
XXXIV IMFP 2006, April 6th
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Page 32
e & μ in
CDF
Central e: ||<1.2
Et>20 GeV
EM cluster + Drift chamber
track,Pt>10 GeV
Loose :
e &  at CDF Run II
Plug e: 1.2<||<2.5
EM cluster (+ Silicon track)
Drift
chamber
High Pt isolated track
(drift chamber)
pointing to a gap in the
- coverage
Tight  :
pointing to a  -stub
ID:
Track quality
|d0|<0.2,0.02 cm
MIP:
Eeom<2 GeV
Ehad<6 GeV
ID:
Ehad/Eem<0.055,
Shower profiles..
E
•Veto cosmics using timing and track information.
•Veto  from jets (mostly b) using calorimeter isolation.
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• Cosq* in Lepton+Jets: (230pb-1)
– 2 Template analysis:
• B tagging used
• Topological variables
W Helicity
• Lepton P
T
in dilepton: (370pb-
1)
– c2 fit is used for lepton
matching (purity: 60%)
Combined result:
f+ = 0.04 ± 0.11 (stat) ± 0.06 (syst)
CDF combined (162pb-1):
0.0<f+<0.25 at 95%CL
0.0<f+<0.27 at 95%CL
f0  0.74
XXXIV IMFP 2006, April 6th
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0.22
0.34
Page 34