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Dynamical Electroweak Breaking @ Dynamical Electroweak Breaking @ LHC LHC Francesco Sannino Francesco Sannino MC-Workshop MC-Workshop Frascati - 2006 Frascati - 2006 The Niels Bohr Institute
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Dynamical Electroweak Breaking @ LHC

Jan 13, 2016

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The Niels Bohr Institute. Dynamical Electroweak Breaking @ LHC. Francesco Sannino MC-Workshop Frascati - 2006. Low Energy Effective Theory. SM. ….is not so standard. Origin of Mass of weak gauge bosons, quarks and leptons is unknown. - PowerPoint PPT Presentation
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Page 1: Dynamical Electroweak Breaking @ LHC

Dynamical Electroweak Breaking @ Dynamical Electroweak Breaking @ LHCLHC

Francesco SanninoFrancesco Sannino

MC-Workshop MC-Workshop Frascati - 2006 Frascati - 2006

The Niels Bohr Institute

Page 2: Dynamical Electroweak Breaking @ LHC

Low Energy Effective TheoryLow Energy Effective Theory

SMSM

Page 3: Dynamical Electroweak Breaking @ LHC

• Origin of Mass of weak gauge bosons, quarks and leptons is unknown.

• Strong Interactions are not fully understood/explored.

• Unnaturally small Neutron Electric Dipole Moment Strong CP problem:

New Challenges from Cosmology.

• Dark Energy/Matter

…….is not so standard.is not so standard

Page 4: Dynamical Electroweak Breaking @ LHC

Strong Dynamics

Focus on two aspects of the SMFocus on two aspects of the SM

Understanding

New

Origin of Mass for the weak gauge bosons, quarks …

as

..and Beyond..and Beyond

Page 5: Dynamical Electroweak Breaking @ LHC

Let there be MassLet there be Mass

Page 6: Dynamical Electroweak Breaking @ LHC

We can already test New Physics! Kennedy,Lynn, Peskin-Takeuchi, Altarelli-Barbieri, Bertolini-Sirlin,

Marciano-Rosner,..:

Electroweak Precision MeasurementsElectroweak Precision Measurements

Page 7: Dynamical Electroweak Breaking @ LHC

Present DataPresent Data

hep-ex/0509008 Now: S = 0.07±0.10

mH=150 GeV

Dutta, Hagiwara and Yan ph/0603038.Weaken constraints

Page 8: Dynamical Electroweak Breaking @ LHC

The Higgs Mechanism in NatureThe Higgs Mechanism in Nature

Page 9: Dynamical Electroweak Breaking @ LHC

SuperconductivitySuperconductivity

Macroscopic-Screening

Non-Relativistic

SM-Screening

Relativistic

Page 10: Dynamical Electroweak Breaking @ LHC

Meissner-Mass

Static Vector PotentialWeak-GB-Mass

Hidden structure ????

Page 11: Dynamical Electroweak Breaking @ LHC

Elementary Higgs: Elementary Higgs:

Trivial and Non-Trivial and Non-naturalnatural

Page 12: Dynamical Electroweak Breaking @ LHC

Natural ScalarsNatural Scalars

Page 13: Dynamical Electroweak Breaking @ LHC

Exact Super Symmetry:Exact Super Symmetry:

Fermions ↔ Bosons

Fermion’s custodial symmetry protects the Bosons

Observe: susy partners

Page 14: Dynamical Electroweak Breaking @ LHC

Composite ScalarComposite Scalar:

Recall Superconductivity

Substructure resolved at scale ΛS

Observe: New Bound States

Page 15: Dynamical Electroweak Breaking @ LHC

Quasi Goldstone Boson:

Protected by spontaneously broken global symmetries.

Near Continuous Quantum Phase Transition

Zero-temperature Bose – Einstein Condensation Lorentz symmetry is broken.

Chiral Phase Transition at zero temperature. Lorentz symmetry is intact.

Page 16: Dynamical Electroweak Breaking @ LHC

Electroweak Symmetry Breaking

@

LHC

Page 17: Dynamical Electroweak Breaking @ LHC

Electroweak Symmetry Breaking

SUSY

Extra Dim.

Technicolor

Curved Flat

Page 18: Dynamical Electroweak Breaking @ LHC
Page 19: Dynamical Electroweak Breaking @ LHC

Technicolor

New Strong Interactions at ~ 250 GeV [Weinberg, Susskind]

Natural to use QCD-like dynamics.

Page 20: Dynamical Electroweak Breaking @ LHC

Problems with the Old Models

• S-parameter: too large

• Large Flavor Changing Neutral Currents (FCNC)

• Limited knowledge of strong dynamics!

Page 21: Dynamical Electroweak Breaking @ LHC

should be sufficiently larger than

Fermion masses versus FCNCFermion masses versus FCNC

PNGMasses

SM-FermionMasses

FCNCOperators

250TC GeV ETC

to reduce FCNC.Progress: Appelquist, Christensen, Piai, Shrok

Page 22: Dynamical Electroweak Breaking @ LHC

Near Conformal Properties

Λ T C

α

q

n o n -c o n fo rm a l

Λ T C

α

qΛ E T C

Λ = 1 0 0 1 0 0 0 E T C - Λ T C

n ea r-c o n fo rm a l

α

β

α *α c

Holdom

Appelquist

Miransky, Yamawaki

Cohen and Georgi…

Page 23: Dynamical Electroweak Breaking @ LHC

Why the walking can help ?

QCD-Like

Near the conformal window

~

~

Page 24: Dynamical Electroweak Breaking @ LHC

Critical Number of techniflavors

For fermions in the fundamental representation near conformal means:

The number of techndoublets is

Page 25: Dynamical Electroweak Breaking @ LHC

The S-parameter for fermions in the fundamental is

Near conformal for N=2 means Nf/2=4 which yields:

Experimentally S = 0.07±0.10

Still too large S-parameter

Appelquist - Sannino

Page 26: Dynamical Electroweak Breaking @ LHC

The New Model

Near conformal for, Nf 2

Small FCNC + Top mass

OK with precision data.

Light Composite Higgs

Dark Matter Sannino-Tuominen, hep-ph/0405209

Hong, Hsu, Sannino, hep-ph/0406200

Dietrich, Sannino and Tuominen, hep-ph/0505059, hep-ph/0510217

Evans-Sannino, hep-ph/0512080

Gudnason, Kouvaris and Sannino, hep-ph/0603014

Page 27: Dynamical Electroweak Breaking @ LHC

The Model: The generalized S-Theory

Page 28: Dynamical Electroweak Breaking @ LHC

Inspired by progress in

Strong Interactions

Page 29: Dynamical Electroweak Breaking @ LHC

`t Hooft - Large N

Corrigan and Ramond `79

Larks

Kiritsis and Papavassiliou `90.

Ryttov and F.S. `05

Helpful for MC ???

Page 30: Dynamical Electroweak Breaking @ LHC

Relation with Super Yang-Mills

A-typeA-typeS-typeS-type

SYMSYM

Armoni-Shifman-Veneziano

Page 31: Dynamical Electroweak Breaking @ LHC

A-type:

QCD vacuum properties, spectrum and confinement/chiral symmetry, finite temperature and density. Armoni-Shifman-Veneziano, Sannino-Shifman, Sannino, (Finite Temperature. Chiral Symmetry vs Confinement) Frandsen-Kouvaris-Sannino (Finite matter density)Sannino-Schechter (..in progress)

N=1 Supersymmetric-Spectrum Merlatti-SanninoFeo-Merlatti-Sannino

Page 32: Dynamical Electroweak Breaking @ LHC

S-type:

Composite Higgs from Higher Representations Sannino

Not ruled out, LCH and DMDietrich-Tuominen-Sannino, Hong-Hsu-Sannino, Sannino-TuominenEvans-SanninoGudnason, Kouvaris and Sannino

Page 33: Dynamical Electroweak Breaking @ LHC

Phase Diagram for the S-Theory

Phase diagram as function of Nf and N. [Sannino-Tuominen]

For N=2,3,4,5 we have that Nf= 2

Page 34: Dynamical Electroweak Breaking @ LHC

Nf=2 & N=2:

Minimal-Walking-Theory

Universal critical number of flavors in the adjoint: Nfc=2.075

Page 35: Dynamical Electroweak Breaking @ LHC

S-parameter

• δ ~ 0.013 due to near conformal dynamics [Sundrum-Hsu, Appelquist-Sannino].

• The estimate for S in the S-type model is:

Page 36: Dynamical Electroweak Breaking @ LHC

Model versus EWPData

68% contour

Electron (m2) and Neutrino (m1) Dirac masses.

Standard Hypercharge Assignment

150 GeV

4th Lepton Family

Page 37: Dynamical Electroweak Breaking @ LHC

A natural LCH*

• Via trace anomaly and the behavior of the underlying beta function near the chiral/conformal phase transition we show:

Page 38: Dynamical Electroweak Breaking @ LHC

Phenomenology of a LCH

Associate Higgs production

Zerwekh 05

Page 39: Dynamical Electroweak Breaking @ LHC

Spectrum

Techni-Mesons

Techni-Baryons Electric Charge

Page 40: Dynamical Electroweak Breaking @ LHC

An Effective Theory

Page 41: Dynamical Electroweak Breaking @ LHC

Some Scenarios

Page 42: Dynamical Electroweak Breaking @ LHC

Dark Side of the 5th Force

NussinovBarr, Chivukula and Farhi

Technibaryon, DD

Universe Charge Neutrality.

Chemical Equilibrium

Taking care of the Sphaleron Processes

Page 43: Dynamical Electroweak Breaking @ LHC

Gudnason, Kouvaris, F.S. ph -0603014

Page 44: Dynamical Electroweak Breaking @ LHC

• MH ~ light

• Fourth Family of Leptons around the Z mass.

• 6 light scalars will be observed.

• Electroweak baryongenesis. Possible Strongly First order phase transition.

• Lattice Simulations are possible

• DM candidate-component

• Unification, Holography….

Predictions and Outlook

Page 45: Dynamical Electroweak Breaking @ LHC

SUSY

TC

LHC

ED

Page 46: Dynamical Electroweak Breaking @ LHC

Spectrum and Effective Theory I

Page 47: Dynamical Electroweak Breaking @ LHC

Spectrum and Effective Theory II

Page 48: Dynamical Electroweak Breaking @ LHC

Small parameters stay small under radiative corrections.

The electron Mass

If set to zero the U(1)L× U(1)R forbids its regeneration

Naturalness begs an explanation of the origin of mass.

No conflict with any small value of the electron mass

NaturalityNaturality

Page 49: Dynamical Electroweak Breaking @ LHC

No custodial symmetry protecting a scalar mass.

A mass appears even if ab initio is set to zero!

Hierarchy between the EW scale and the Planck Scale.

No!No!

Is the Higgs Natural?Is the Higgs Natural?