theory of electroweak interactions

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Theory of Electroweak Interactions Open KIAS PCSI, 2013 Theoretical structure Discovery of W and Z Quantum fluctuations [Okun, Leptons and Quarks] [Perkins, Introduction to HEP] [Peskin, Perimeter, 2009] [Altarelli, arXiv:1303.2842] [Quigg, ICTP-SAIFR School, 2013] [EW review, PDG 2012] [Higgs review, PDG 2012]

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Page 1: Theory of Electroweak Interactions

Theory of Electroweak Interactions

Open KIAS PCSI, 2013

Theoretical structure Discovery of W and Z Quantum fluctuations

[Okun, Leptons and Quarks] [Perkins, Introduction to HEP]

[Peskin, Perimeter, 2009] [Altarelli, arXiv:1303.2842]

[Quigg, ICTP-SAIFR School, 2013] [EW review, PDG 2012]

[Higgs review, PDG 2012] …

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[Perkins, Intro. to HEP]

Milestones in Particle Physics

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X ⇔ Y

1973

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FB Asymmetry Two-fold ambiguity disappeared!

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CC NC

[Weinberg’s nose]

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Discovery of Z and W

Z boson

1983

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W boson

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Production of Z at LEP I & SLC and W pair at LEP II

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+

Precision tests of the Z sector

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Z-boson pole

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Z lineshape

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Identical resonance, independent of final states ⇒ same propagator

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Principal Z pole observables

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Number of light neutrino families

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Precision tests of the W sector

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W branching ratios

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W mass measurements

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Triple gauge couplings

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EW unification seen at HERA

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Top quest

Raison d'être

Two families cannot account for CP violation in the quark sector

Given the existence of b and τ, the top quark is requested for

anomaly cancellation

Absence of FCNC in (tree-level) b decays

b quark has a weak isospin of -1/2, demanding a partner

[Schaile and Zerwas, 1992]

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Higher-order corrections ⇔ Top (and H) mass

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Global fits to precision EW measurements

Precision and calculations improve with time!

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Observation of the top quark at Tevatron (1995)

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Successful SU(2) x U(1) EW structure

NC Charm W & Z

Precision EW tests (0.1%)

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H influence

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Higgs Odyssey

A Higgs boson SM Higgs or not?

Implications Prospects

Discovery of a new boson on July 4, 2012

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Characteristic 2 γ and 4μevents

[CMS]

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[ATLAS]

Accumulated 2-photon and 4-lepton events

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mH = 125.4 0.5 (stat.) 0.6 (syst.)

With additional data, new analysis, significance decreased relative to July/4!!

CMS HIG-13-001

7.4σ

ATLAS-CONF-2013-021

7.4σ (obs) ⇔ 4.1σ (exp) m

H = 126.8 ± 0.2(stat) ± 0.7(syst) GeV

Moriond 2013 [Incandela @ Princeton] H

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H Z*Z 4 l

6.7 s (obs) ⇔ 7.1 s (exp) = s/sSM = 0.92 ± 0.28

CMS HIG-13-002

6.6σ (obs) ⇔ 4.4σ (exp) m

H = 124.3 ± 0.6

0.5 ± 0.5

0.3 GeV

µ = 1.7 ± 0.50.4

ATLAS-CONF-2013-013

Moriond 2013

[Incandela @ Princeton]

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H tt

m = 120+9-7 (stat+syst) GeV CMS HIG-13-004

~3 s

First strong indication of decay to spin ½ particles

μτh, eτh, eμ, τhτh, μμ

Moriond 2013

[Incandela @ Princeton]

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SM Higgs Couplings

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Basic Diagrams for the SM Higgs Boson

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Production Decay SM Higgs

Clean signature

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Signal strength and mass (combining and ZZ*)

=0.80±0.14 =1.30±0.20

m = 125.7 ± 0.3 ± 0.3 GeV m = 125.5 ± 0.2 +0.5-0.6 GeV

CERN 4/15, 2013

[Incandela @ Princeton]

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The SM Higgs Boson ?

A Higgs Boson !

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RGE running of the quartic Higgs coupling

QFT vacuum is a dielectric medium that screens charge ⇒ the effective charge is a function of the distance or the energy.

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Triviality : MH from above

If the SM is valid to infinite energy, thenλ(v2) =0, i.e. non-interacting.

Since the Higgs mass is non-zero, then the theory has a cutoff ΛC

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Stability : MH from below

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Message

For any Higgs mass, there is a maximum energy scale beyond

which the theory ceases to make sense.

The description of the

Higgs boson as an elementary scalar is at

best an effective theory, valid over a finite range of energies.

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Extremely sensitive to the top quark mass

Meta-stable vacuum

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New Endless Issues?!

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[Haber]