Prospects of Top Quark Properties @ ATLAS
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Transcript of Prospects of Top Quark Properties @ ATLAS
RHUL-Royal Holloway, University of London: 16th November 2007
Prospects of Top QuarkProspects of Top QuarkProperties @ ATLASProperties @ ATLAS
A.Onofre A.Onofre ([email protected])([email protected])
RHUL-Royal Holloway, University of London: 16th November 2007
Top Properties (T7 CSC Note+ST)
Outline
Top Mass Top Charge Top Spin and Spin Correlations Top tWb decay tt Resonances Top FCNC decays Single Top FCNC Production
Conclusions
RHUL-Royal Holloway, University of London: 16th November 2007
2 b-jets
pT>20GeV
pT>20GeV
≥4 jets,R=0.4 pT>40GeV
t(had)
t(lep)
W(had)
Semileptonic TopologySemileptonic Topology Dileptonic TopologyDileptonic Topology
e,
e,
b
b
W
W
2 b-jets
2 leptons
Studies done with tt Events
Top Mass, Top Charge, Top Spin and Spin Top Mass, Top Charge, Top Spin and Spin Correlations, Top tCorrelations, Top tWb decay and tt Wb decay and tt ResonancesResonances
Top FCNC decays (tTop FCNC decays (tqX, X=qX, X=,Z,g) and Single-,Z,g) and Single-toptop
RHUL-Royal Holloway, University of London: 16th November 2007
Top Mass
Many analyses performed in the past or being developed recently:
Cut based Kinematic fit Template method, Matrix Element method, Analyses with soft muon b-tagging, high pT top, Analysis in leptonic final states with J/ Correlation between lepton pT and mt
RHUL-Royal Holloway, University of London: 16th November 2007
Top Mass
SACLAY Analysis: choice of light jet pair and in-situ re-calibration using a 2 fit to the PDG W mass
Systematic uncertainties: Jet energy scale
1% on light jet 0.2 GeV/c2 on mt
1% on b-jet 0.7 GeV/c2 on mt
ongoing ISR/FSR , b-quark fragm.
Efficiency* 3.44 ± 0.04%
S/B 100 ± 11
Purity 63.8 ± 0.8 %
<Mtop> 175.8 ± 0.4 GeV/c2
FULLSIM (CSC) L=1fb-1
(SN-ATLAS-2004-040)L=10fb-1 ATLFAST (reminder)
Tot(sys) = 1.3 GeVTot(stat) = 0.1 GeV
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Top Charge
Exotic
t(-4/3)
b(-1/3)
W-
l-(-1)
lSM
t(2/3)
b(-1/3)
W+
l+(+1)
l
SM SM ((QQtoptop==++2/32/3): ): ExoticExotics s ((QQtoptop= -4/3= -4/3):):
13/13/2 Wbt13/13/4ˆ Wbt
1el
1el
Critical momentCritical moment For top quark determinationFor top quark determination
I) Determination of b-jet chargeI) Determination of b-jet chargeII) Correct (lepton, b-jet) pairingII) Correct (lepton, b-jet) pairing
(Atl(Atlfastfast, , PHYS-2003-35)PHYS-2003-35)
RHUL-Royal Holloway, University of London: 16th November 2007
Top ChargeI) Determination of b-jet Charge:I) Determination of b-jet Charge:
II) Correct (lII) Correct (l±±, b) Pairing:, b) Pairing:
m( l ,b2 )
m( l , b1 )
Mtop=175 GeV
A) Weighting Technique:A) Weighting Technique:
Ni
k
i
Ni
k
iijetb
pj
pjqQ
B) Semileptonic B) Semileptonic Decay:Decay:
ljetb qQ
Invariant mass Invariant mass criteria:criteria:
b1
b2
l
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Top Charge(B.Zilka,S.Tokar)
A) Weighting Technique:A) Weighting Technique:b
b
-0.0842 -0.0842 0.0044 0.0044
0.0868 0.0868 0.0043 0.0043
( Eff.=4.1% Purity: 89.3% )
L~0.5fb-
1
B) Semileptonic Decay:B) Semileptonic Decay:(A. Tonoyan, E.Khramov)
l+l+
l-l-
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Top Spin and Spin Correlations
LO) (SM0.31)σ()σ()σ()σ()σ()σ()σ()σ(
A
Mtt<550 GeV A=0.42
Double Angular Distributions:
Mtt<550 GeV AD =-0.29
tt Spin Correlation Parameters: Although t and t not polarised in tt pairs, their spins are
correlated
)coscos1(4
1
)(cos)(cos
1 2
XXXXXX
Add
d
)cos1(2
1
cos
1XXXXD
XX
Ad
d
(Zhu Chengguang)
RHUL-Royal Holloway, University of London: 16th November 2007
Top Spin and Spin Correlations
Semileptonic + Dileptonic Syst (Eb-jet,mtop,FSR) 4-6% precision
(Eur.Phys.J.C44S2 2005 13-33)L=10fb-1 ATLFAST (reminder)
FULLSIM (CSC) L=1fb-1
SemileptonicSemileptonicSelection efficiency 2.9% (2.7% for Rome)
Preliminary
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Top Spin and Spin Correlations
Trigger Studies:
Isolated single electron trigger
Single muon trigger
L=1fb-1
Results (Preliminary):
Level of Precision of A, AD
~40%
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Spin Asymmetries can also be used:
Error versus Luminosity:SM (LO): Alj=-0.0396
spin analysing power l+=1.0, j=-0.51)
Alj
L=1fb-1
Level of Precision of Alj~40% (Low MC)
Alj~30% (High MC)
0)N(0)N(
0)N(0)N(
XXXX
XXXX
cosθcosθcosθcosθ
cosθcosθcosθcosθ
ˆˆ
ˆˆ
0)N(0)N(
0)N(0)N(
XXXX
XXXX
coscos
coscos
ˆˆ
ˆˆ
Top Spin and Spin Correlations
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Top Decays: 1) the ttWbWb decay
By measuring the fraction of longitudinal W´s in top quark decays we are:
V-A S
UPPRESSED
Testing a Standard Model prediction: F0=0.7 FL=0.3 Probing the structure of the Wtb vertex
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Top tWb decay (SM)
Angular Distribution @ W c.m.
How to measure the W Helicity Fractions?
Using lepton angular distribution (with respect to top direction) in W cm system:
SM(LO): F0=0.703 , FL=0.297 , FR=3.6x10-4
(NLO): F0=0.695 , FL=0.304 , FR=0.001cos(l*)
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(Eur.Phys.J.C44S2 2005 13-33)L=10fb-1 ATLFAST (reminder)
• Syst ( Eb-jet,mtop,FSR )• F0 F0 ~ 2% ; FR ~ 0.01
FULLSIM (CSC) L=1fb-1 Results (Preliminary)
• F0 F0 ~ 6% ; FR ~ 0.03
(Zhu Chengguang)
Top tWb decay (SM)
(CDF) First Simultaneous fit:
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Anomalous Couplings @ the Wtb Vertex
VR,gL,gR Change F0,FL,FR
How to Probe Anomalous Couplings?
• Extract Limits from F0,FL and FR (and ratios) • Fit angular distr. with VR, gL and gR (mb≠0)• Use Angular Asymmetries
Eur.Phys.J. C50 (2007) 519-533
Top tWb decay (BSM)
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Angular Asymmetries:
(NLO): AFB=-0.2269 , A+=0.5429 , A-=-0.8402
(SM, LO): AFB=-0.2225 , A+=0.5482 , A-=-0.8397
Top tWb decay (BSM)
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Anomalous Couplings
Asymmetries
(N. Castro)
Error Versus
Luminosity
A+A-
Top tWb decay (BSM)
L~1fb-1 L=10fb-1
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Discovery Potential of a Narrow tt Resonance
(E.Cogneras,D.Pallin)tt Resonances
Discovery Potential: Window in mass spec. Compute the number of resonance events required for discovery: nX = 5 deviation on nSM
SemileptonicSemileptonic
Resolution
Current Limits:
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L=10fb-1 ATLFAST (reminder)
Expected 95% CL Limits:
Br(tqg) <1.3x10-3 5 Results:
Br(tqZ) >4.4x10-4
Br(tq) >9.4x10-
5
Br(tqg) >4.3x10-3
(SN-ATLAS-2007-059)
Top FCNC decays
FCNC in tt Events
tqZ tqgtq
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FULLSIM L=1fb-1
Results Crucially Depend on Tagging Efficiencies (e, , b, jets and )
Likelihood Method works (need to have well defined shapes)
Gluon Channel more difficult
(F. Veloso)
5 Results:
Br(tqZ) ~ 10-2 - 10-3
Br(tq) ~ 10-3
Br(tqg) ~ 10-2
Top FCNC decays
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FULLSIM L=1fb-1
(F. Veloso)
5 Results:
Br(tq) ~ 10-3
Top FCNC decays (w/o b-tag)
Minimize 2 by looping on jets (b,q=j1,j2) and scan on p
Z to reconstruct kinematics
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FCNC in Single-t Production
kkqgqg=anomalous coupling =anomalous coupling =scale of new =scale of new physicsphysics
Event Selection: 1 lep ( pT>20GeV, <2.5 )
1 b-jet ( pT>40GeV, <2.5 )
pT > 20GeV
( W and t p( W and t pTT, m, mblbl, m, mTT(W), H(W), HTT, m, mtt ) )
Systematics:signal signal (8%), b(8%), btagtag (6%), ISR (3.5%), (6%), ISR (3.5%), PileUp (4%) PileUp (4%) Total ~ 12%Total ~ 12%
(ug)=1.08%, (cg)=1.81%Back: W+j(80%), single-
t(9%)
L=10fb-1 ATLFAST (reminder)
Results:
(hep-ex/0702005)
Br(tug)~O(10-3)
Br(tcg)~O(10-2)
Estimate:
“Direct”
(T.L. Cheng, P.Teixeira Dias)
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The Direct Production is not the full Story
FCNC in Single-t Production
The ggqt Processes:
The gqgt Processes:
The X-section:
The X-section:
Phys.Rev. D74 (2006) 014006
(R.Santos, P.Ferreira)
RHUL-Royal Holloway, University of London: 16th November 2007
FCNC in Single-t Production
Just To Have an Idea of the Results for :
5 and 95% CL Limits obtained
L=10fb-1
5 Discovery 95% CL Limit: 95% CL Limits:Br(tqg) ~O(10-4)
5 Discovery:
Br(tqg) ~O(10-3-10-4)
New Contributions Give Same Order of Magnitude Results as Direct Production Mechanism 1 Order of magnitude better than ttbar for the gluon channel
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Conclusions Atlas will perform precision studies in the top sector
Several Methods Available to Extract Physical Observables
Already @ 1fb-1: Top Mass ~ O(few GeV/c2) Top Charge (2/3 versus -4/3) > 5significance Spin Correlation Parameters (A,AD) ~ 40% error Spin Asymmetries ~ 40% error W helicity fractions (F0, FL, FR ) ~ 6%, ~10% and ~0.03 error Angular Asymmetries (A+,A-) ~ 3% and 1% error Anomalous Wtb Couplings (VR, gL, gR ) ~ 0.1, 0.05 and 0.03 error tt Resonances (1TeV) ~ (×Br)≥ 8 pb FCNC top Decays (Br[tqX], X=,Z,g) ~ 10-2 - 10-3
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Next Top Workshop(every 2 years)
2008
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Spare Slides
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Top Mass @ TEVATRON
RHUL-Royal Holloway, University of London: 16th November 2007
tt @ TEVATRON