Status of Single Top Searches at the Tevatron - PowerPoint PPT Presentation

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Status of Single Top Searches at the Tevatron

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TEV4LHC Workshop, Fermilab, ... Current Searches for Single Top Quark Production at D and CDF ... (lepton) MET SiET(jeti) M(top) t-channel: ... – PowerPoint PPT presentation

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Title: Status of Single Top Searches at the Tevatron


1
Status of Single Top Searches at the Tevatron
  • Reinhard Schwienhorst

TEV4LHC Workshop, Fermilab, September 16 2004
2
Outline
  • Introduction
  • Standard Model Single Top Quark Production
  • Event Signature
  • Backgrounds
  • Current Searches for Single Top Quark Production
    at DØ and CDF
  • Sensitive Variables
  • Current results
  • Analysis Status and Outlook
  • The Phenomenological Connection
  • Conclusions
  • Notes
  • I will not discuss LHC Single Top searches
  • I will not discuss non-SM Single Top

3
SM Single Top Quark Production at the Tevatron
t-channel
s-channel
t
q
q
q'
W
W
b
t
g
?q'
?b
Vtb
?b
  • Electroweak (charged current) production of top
    quarks
    s-channel
    t-channel st channel
  • NLO cross-sections 0.88pb 8
    1.98pb 11
  • Run I 95 CL limits, DØ lt17pb
    lt22pb
    CDF lt18pb
    lt13pb lt14pb
  • Tevatron Goal Measure CKM matrix element Vtb
    (test CKM unitarity)
  • Observe top polarization
  • Discover new Physics
  • Additional production mode at the LHC Wt
  • Not discussed here (sTEV0.09pb)

Wt
W
b
t
g
4
Identifying Single Top Events
b
  • Event signature
  • Similar to top pair production in the leptonjets
    channel
  • But fewer jets
  • Larger Backgrounds
  • Similar to associated Higgs production
  • Single top s-channel is an important background
    to Higgs searches at the Tevatron
  • Important Tools
  • Good lepton ID
  • Reduce fake-lepton backgrounds
  • 1 high-ET lepton
  • ET
  • ?2 jets
  • ?1 b-tagged jets

l
t
/
n
?b
  • Excellent b-quark tagging
  • Good jet ID and resolution

5
Standard Model Backgrounds
l
W
  • W/Zjets production (real-l)
  • Wjj, Wcc, Wbb, Zjj, Zcc, Zbb, ...
  • Estimated from data (DØ)
  • Estimated from MC/data (CDF)
  • Mis-reconstructed multi-jet events (fake-l)
  • Jet mis-identified as isolated electron or muon
  • Estimated from data
  • Top-pair production
  • Estimated from MC
  • Other (WZ, WW, Ztt, cosmic rays,...)
  • Estimated from MC (CDF)
  • Included in data W/Zjets estimate (DØ)

n
q
q (b)
g
?q'
q (b)
l
n
q
t
b
?q'
?b
?t
g
q
q
6
Analysis Strategy
  • Loose pre-selection cuts
  • Lepton, MET
  • ETgt15GeV (DØ), ETgt20GeV (CDF)
  • Jets ETgt15GeV (DØ and CDF)
  • Large h range, maximize acceptance
  • B-tag requirement
  • Check background model
  • Final Event Selection
  • Tight cuts to separate single top signal from
    backgrounds
  • Separately for s-channel and t-channel
  • and st combined
  • Cross Section (limit) derivation
  • Event counting (DØ)
  • Template fit (CDF)

7
Variables used in the analysis
  • Initial analyses are using simplevariables for
    cuts or fits
  • HTET(lepton) MET SiET(jeti)
  • M(top)
  • t-channel pseudorapidity of the light quark jet
    lepton (top) charge

8
Current Results (160-170pb-1)
DØ Run II preliminiary
b-tagging algorithm
Yields SLT SVT JLIP Signals
s-channel 1.30.3 3.10.8 3.20.7
t-channel 1.70.4 5.11.3 5.31.3 Background
sum 7613 13721 16626 Observed 97 138 148
Systematic Uncertainties MC signal JES, trigger
and tagger modeling, (DØ 20, CDF 10acc,
20-30 shape) MC backgrounds also normalization,
25 ? nuisance parameter in template fit Data
backgrounds DØ dominated by tagging probability
estimate, 20
Observed/Expected limit at 95CL
st lt 10 /11 pb
ss lt 14 /12 pb
st lt 25 / 23 pb
ss lt 19 / 16 pb
sst lt 18 /14 pb
sst lt 23/20 pb
9
Analysis Status and Outlook
  • Initial analysis started after Run II top pair
    production observation
  • Current Results are already an improvement over
    Run I limit
  • More data, better detector
  • Current analyses would need several fb-1 for
    observation
  • Particle ID, b-tagging not as efficient as
    predicted
  • Improvements in progress
  • Large systematic uncertainties
  • Background modeling, detector understanding, ...
  • Analyses are not yet optimized
  • Working on multivariate analysis techniques (NN,
    Matrix Element, ...)
  • Required to make observation soon
  • Need accurate models for signal and background
  • Benefit from recent NLO calculations
  • Identify variables that give good
    signal-background separation

10
The Phenomenological Connection
Tevatron
LHC
Phenomenology
  • Phenomenological studies provide important
    information
  • Cross sections, Distributions, correlations,...
  • How to combine the different t-channel diagrams
    in a generator
  • Several recent phenomenology papers on single top
    at NLO at the Tevatron, more papers in
    preparation
  • Address signal and background issues
  • Studies of single top production (Z. Sullivan)
  • Single top production and decay at
    next-to-leading order (J. Campbell, R.K. Ellis,
    F. Tramontano)
  • Next-to-leading Order Corrections to Single Top
    Production and Decay at the Tevatron 1.
    s-channel Process (Q. Cao, RS, C.-P. Yuan)

11
Example Cross Section and Jet multiplicity
t-channel
s-channel
total cross section
s-channel
t-channel
fraction of 3-jet events
12
NLO distributions of 3rd jet
t-channel
s-channel
s-channel
t-channel
13
Conclusions
  • Tevatron single top analyses have started
  • Focus on understanding data
  • First results are improvements over Run I limits
  • Improvements to the analysis are needed for
    observation
  • Implement more advanced final analysis steps
  • Reduce systematic uncertainties
  • Improve efficiencies ID, b-tagging, trigger, ...
  • In progress
  • Cooperation with Phenomenologists is important
  • Model signal accurately
  • Model backgrounds accurately
  • New ideas for sensitive variables

Single Top Physics at the Tevatron is
challenging and will be a very active field for
the next few years
14
Backup Slides
15
Event pre-selection
  • Loose cuts to select events with lepton,
    neutrino, jets DØ
    CDF
  • Lepton ETgt15GeV
    ETgt20GeV hdetlt1.1 (e)
    hdetlt2.0 (m) hlt1.0
  • Neutrino ETgt15GeV
    ETgt20GeV
  • Jets 2?njets?4
    njets2
    ETgt15GeV
    ETgt15GeV hdetlt3.4
    hlt2.8
    ET(jet 1)gt25GeV
  • b-tag use 3 different taggers
    require secondary vertex tag

/
/
muon-in-jet
secondary vertex
impact parameter
16
Final Event Selection
  • Separate s-channel production (2 b-tagged
    jets)from t-channel production (1 b-tagged jet)
  • Reconstruct top quark
  • Cut on invariant mass of lnb system
  • Cut on variable that separates signal and
    dominant background
  • Total event transverse energy HT

CDF Run II preliminary
Mlnb GeV
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