Download - EW observables probe the Higgs bosons indirectly by means of quantum corrections .

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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) ?