d u +-strom i wk + u d --strom i wk - d(u) u(d) 3-strom i wk 3 w-w- w+w+ w3w3 n p +-strom + p n...

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d u “+”-Strom I wk + u d “-”-Strom I wk - d(u) u(d) “3”-Strom I wk 3 W - W + W 3 n p “+”-Strom + p n “-”-Strom - n(p) p(n) “3”-Strom 3 - + 0 Parallele starker-schwacher Isospin: 3 , 3 , , , , ' , ' , : , : wk wk wk weak stark I I I s c d u l I d u n p I Folgerung GIM: Wenn schwache WW sich als SU(2) beschreiben laesst, dann muss es auch neutrale Stroeme geben!

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Page 1: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher

d

u

“+”-Strom

Iwk+

u

d

“-”-Strom

Iwk-

d(u)

u(d)

“3”-Strom

Iwk3

W- W+ W3

n

p

“+”-Strom

+

p

n

“-”-Strom

-

n(p)

p(n)

“3”-Strom

3

- + 0

Parallele starker-schwacher Isospin:

3,3 ,,,,

',

',:,:

wkwkwk

weakstark

III

s

c

d

u

lI

d

u

n

pI

Folgerung GIM:Wenn schwache WW sich als SU(2)beschreiben laesst, dann muss es auch neutrale Stroeme geben!

Page 2: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher
Page 3: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher
Page 4: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher

CDF and DØ in Run II

New Silicon DetectorNew Central Drift ChamberNew End Plug CalorimetryExtended muon coverageNew electronics

Silicon Detector2 T solenoid and central fiber trackerSubstantially upgraded muon systemNew electronics

Driven by physics goals detectors are becoming “similar”: silicon, central magnetic field, hermetic calorimetry and muon systems

DØØ CDF

Page 5: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher

Top Quark Production and Decays

Top quarks at Tevatron are (mainly) produced in pairs via strong interaction

Top pair cross section at 1.96 TeV is 6.7 pb

In SM top decays 100% to WbClassification of top decays

is based on Ws decays

% e qq

e 1.2 2.5 2.5 14.8

1.2 2.5 14.8

1.2 14.8

qq 44.4

classification: di-lepton, lepton+jets, all jetsTwo b quarks in final state!!!

85%

15%

Page 6: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher
Page 7: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher

Detection of High Pt Objects

Electrons

Missing Et

Muons

Top and Higgs final decay products

electrons muons jets (b)

missing Et ()Detection and MC

optimization using well known objects

Page 8: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher
Page 9: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher

Selection of Top Quark Events

In triggering and analysis select events with high Pt leptons high Et multiple jets large missing Et () displaced vertex for b jets

“Di-lepton” mode has low backgrounds: di-bosons, Drell-Yan, ... but low statistics: ~5% for e, decays“Lepton+jets” very productive mode 6 times more decays then di-lepton mode main background W+jets good purity after b tagging“All jets” mode ~50% branching high QCD backgrounds, jets combinatoric

Page 10: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher
Page 11: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher
Page 12: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher
Page 13: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher

Run II Top Mass at CDFdi-leptons

l+jets, b tagged

l+jets GeV )(9.6)(5.176 2.170.16 syststatmt

GeV )(5.6)(9.174 1.77.7 syststatmt

GeV )(8.6)(6.179 4.63.6 syststatmt

… erst gut durch Kombinationvieler einzelner Analysen

Page 14: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher

Run II Top Quark Cross Section

Measurements demonstrate success of multiple top detection techniquesResults within errors consistent with NNLO SM predictions for 1.96TeV of 6.7pb

Page 15: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher

Tevatron Top Quark Mass

mt = 178.04.3 GeV

Run II top quark mass results from both detectors are available

TeV EWWG is working on combining Run II top mass measurement from CDF and DØØ

Systematic error (mainly jet energy scale)

is becoming limiting accuracy factor

Page 16: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher
Page 17: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher
Page 18: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher

Resonances in tt system?

MX > 560 GeV

No resonance production in tt system is expected in SM

Some models predict tt bound states, example: topcolor-assisted technicolor predicts leptophobic Z’ with strong 3rd generation coupling

Experimental check: search for bumps in tt effective mass spectrum

DØ, 125 pbØ, 125 pb-1-1

Background

Top

Total

Page 19: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher
Page 20: D u +-Strom I wk + u d --Strom I wk - d(u) u(d) 3-Strom I wk 3 W-W- W+W+ W3W3 n p +-Strom + p n --Strom - n(p) p(n) 3-Strom 3 - + 0 Parallele starker-schwacher