ew observables probe the higgs bosons indirectly by means of quantum corrections

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EW observables probe the Higgs bosons indirectly by means of quantum corrections. Large quantum corrections to EW observables come from the top quark. Electroweak Measurements

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Electroweak Measurements. EW observables probe the Higgs bosons indirectly by means of quantum corrections . Large quantum corrections to EW observables come from the top quark. M top : Direct vs. Indirect. Indirect meas.s : fits to EW observables. Direct meas.s : CDF and D0. - PowerPoint PPT Presentation

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Page 1: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

EW observables probe the Higgs bosons indirectlyby means of quantum corrections.

Large quantum corrections to EW observables come fromthe top quark.

Electroweak Measurements

Page 2: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

Mtop : Direct vs. Indirect

Indirect meas.s :fits to EW observables

Direct meas.s :CDF and D0

Lower limits : direct searches in e+e- and pp

Page 3: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

MH < 165 ~ 206 GeV at 95% CLFavor light Higgs

Precision EW Measurements

Page 4: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

Mw(GeV)

MH(GeV)

Mtop (GeV) year

1 prediction

1991 Mtop limit

1991

2001

1995

EW Measurements (last ~10 years)

Page 5: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

Higgs Searches at LEP 2 (e+e- collider)

e+e- ZHcross section (fb)

e+e- cm energy (GeV)

M > 109 GeV3.0 ZH, 3.6 bgrn, 6 observed

~2 excess observed in agreement with MH ~ 115 GeV

or MH > 113 GeV at 95% CL

Page 6: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

& girls

TevatronLEP 2

Higgs Searches : LEP 2 Tevatron

Page 7: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

Run IIa

Tevatron Run IIa EW Measurements

Page 8: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

Tevatron & CDF/D0 Upgrade (Run II)

HW+

W-Hd-

u

W+*

W+

LEPReach

t

Page 9: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

Run IIa2001 ~ 2003 : 2fb-1

Run IIb2004 ~ 2007 (?)

20fb-1 (?)

Page 10: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

installing silicon tracker, prior to detector roll-in

CDF Detector

Page 11: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

electronics

1.5m

~722 k channels

silicon

CDF Silicon System

Page 12: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

residual dist. (cm)

Hit Resolution~200 m

Goal : 180 m

96 layers

e+

e-

CDF Drift Chamber

a collaboration of several groups includingY.K.Kim’s group (Berkeley)

Page 13: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

Ko p B+ J/ K+

Z e+ e- Jets

J/ +-

() GeV/c2

W e transverse mass

CDF : Preparing for First Physics …

Page 14: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

Ko p B+ J/ K+J/ +-

() GeV/c2

Page 15: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

CDF B Signals

Page 16: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

CDF B Signals

Page 17: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

CDF Z Signals

Page 18: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

CDF Z Signals

Page 19: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

CDFJets

Page 20: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

Physics with 200 pb-1

B physics BS mixing sin2

Top, EWK physics a larger sample

~ (Run I) x 4

Extend SUSY and new particle studies

QCD

BS DS , DS DS

SM

discovery

hint

Near-term Prospects

Page 21: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

the Standard Model Its foundation is symmetry. Effective Theory

Supersymmetric extensions of the Standard Model Supersymmetry relates bosons

and fermions. h, H, A, H+, H-

h SM Higgs Mh < ~130 GeV

Grand Unified Theory Unification of

coupling strengths

Physics beyond the Standard Model

Evolution of EM, Weak, Strong

SM

SUSY

~~

e+ e-

superparticle

e e~

e

Me Me

Page 22: EW observables probe the Higgs bosons indirectly by means of  quantum corrections

necessary to understand EWSB

1991 2021 (year)

LEP (e+e-) 208 GeV

LHC (pp) 14 TeV

Tevatron (pp) 2 TeVRun IIRun I

Energy Frontier Acceleratorsto understand origin of Mass

2001 2011

e+e-(0.5-1 TeV) ?

e+e-, +- (2-4 TeV) ?pp (~100 TeV) ?