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Top Quark Physics. Suyong Choi Korea University. Top Quark in the Standard Model Measurement of Production C ross S ections Properties of the Top Quark Summary and Outlook. Contents. Top quark in the Standard model. Discrete quantum numbers Spin Weak i sospin Charge Mass
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Top Quark Physics Suyong Choi Korea University
Top Quark in the Standard Model • Measurement of Production Cross Sections • Properties of the Top Quark • Summary and Outlook Contents
Discrete quantum numbers • Spin • Weak isospin • Charge • Mass • Lifetime or Decay width • Branching fraction • Coupling – QCD, EW Properties of Top Quark
Top quark carries “color” and interacts with gluons • Production of top quark pairs is important probe of QCD interactions QCD
Fermion part • Interaction with H, W, , Z Electroweak Lagrangian
Strong interaction: • Coupling to neutral gauge boson: • Coupling to charged gauge boson: • Coupling to Higgs field (boson): • Coupling to Higgs field: Interactions of Top Quark in SM
Decays to physical states • Top decays almost 100% to W+b Top Quark Decays
1.3 GeV width for 172 GeV top quark • s • Top quarks are produced and decay like free quarks with spin at production information intact • Hadron formation time • Hadron formation is governed by light-quark dynamics • In contrast, B mesons decay isotropically Top Decay Width
Top quark polarization is reflected in angular distribution of decay products Polarized Top Quark
Radiative corrections to W and Z propagator • Quadratic sensitivity to fermion masses Top Quark Corrections to Electroweak Measurements
W and Z masses • Z mass was measured very precisely at LEP experiments • could be inferred with knowledge of • Test of EW theory Top Quark and Electroweak Measurements
Top quark mass could bepredicted from precisionmeasurements Prediction from LEP
CDF DØ CDF DØ Top Quark Run 2 results Top Mass Distributions from 1995 observation paper
LEP EW precision results from Top Quark Mass from Electroweak Data
In conjunction with W and Z,we can gain information on Higgs mass Connection with Higgs
Top quark is special • Most massive • Interaction only within 3rd generation • top-Higgs coupling ~ 1 • Boundary between metastabilityand stability The Top Quark
5 fb-1 @ 7 TeV 20 fb-1 @ 8 TeV LHC and Experiments
Properties • Mass • Decay width • Spin • Coupling • Cross section measurements • Production and decays Physics with Top Quarks
Higher cross sectionand higher luminosity at LHC • Top quark factory • Rare processes with top quarks • New physics with top quarks • Tevatron and LHC are complementary Cross Sections at Tevatron and LHC
Strongly produced • Contribution of andchanges as Pair production diagams Pair Production
Lepton+jets per lepton flavor Multijet – Highest statistics, but large backgrounds and combinatorics Lepton+jets – Highest statistics and usually yields best measurement Dilepton – Smaller statistics but clean, less combinatoric, solving for 2 neutrino momenta not trivial channels
Lepton+Jets • 1 charged lepton • 4 hadronic jets (2 are b-quark jets) • Missing ET • Problem • How to correctly assign jets to top or antitop • How to reconstruct neutrino momentum Reconstructing tt-bar Events
1 unknown: neutrino • , • 3 constraints: • Problem of combinatorics • 2 fold ambiguity – if 2 b-jets tagged • 6 fold ambiguity – if 1 b-jet tagged Top Quark Reconstruction in L+Jets
Have to consider • experimental uncertainties on measurements • finite widths of W and top • Numerically minimize event-by-event Top Quark Reconstruction in L+Jets
Experimental error comparable to theory error • QCD explains well the inclusive pair production Pair Production Cross Section
s and t channel • Electroweak production • Cross section of the sameorder as pair production • Sensitive probe of withoutthe assumption of 3 generationof quarks W associated Single Top Production
Signal Region Control Region significance Observation of Wt Single Top Production
From single top quark production cross section, we can measure directly without assuming 3 generation of quarks • Current best direct measurement: Measurement of
Tevatron: GeV– 0.5% accuracy Mass of Top Quark
CPT violated if • and distinguished by electric charged of lepton Mass Difference of and
In SM, top quark width at NLO is • 1.29 GeV/c2 • Lifetime of • Decay width reflected in reconstructed mass distribution • CDF measures Decay Width of Top Quark
B-jet charge calculatedfrom tracks associatedwith b-jet Electric Charge of Top Quark
Use lepton angular distribution in top rest frame • W from top decays are either left-handed or longitudinal W Polarization from Top
On average, spin of top and antitop are unpolarized, but event-by-event, their spins are correlated • Most prominent in initial state: aligned top spin • For gg mostly anti-aligned spins • Results depend on spin quantization axis chosen Relativistic top Produced at Rest Spin Correlation in Production
and the spins of top quarks are correlated • Due to , spin state of top at production reflected in decay products • Lepton is the most sensitive probe of top spin polarization • Tevatron and LHC has different contributions of and • ATLAS observed spin correlations at 5.1 s.d. Spin Correlation
Major background to • Number of b-tagged jets distribution Production
Anomalous Single Top Search for Search for FCNC
Top-Higgs coupling almost 1 • Consistent with backgrounds • Cross section limits at Search for
Approaching 20 years of rich physics program at hadron colliders with top quark events • Top quark production and properties consistent with SM • Many measurements systematics limited. What can you do with millions of top quark events? Summary and Outlook