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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

Dynamical Electroweak Breaking @ LHC

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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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Dynamical Electroweak Breaking @ Dynamical Electroweak Breaking @ LHCLHC

Francesco SanninoFrancesco Sannino

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

The Niels Bohr Institute

Low Energy Effective TheoryLow Energy Effective Theory

SMSM

• 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

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

Let there be MassLet there be Mass

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

Marciano-Rosner,..:

Electroweak Precision MeasurementsElectroweak Precision Measurements

Present DataPresent Data

hep-ex/0509008 Now: S = 0.07±0.10

mH=150 GeV

Dutta, Hagiwara and Yan ph/0603038.Weaken constraints

The Higgs Mechanism in NatureThe Higgs Mechanism in Nature

SuperconductivitySuperconductivity

Macroscopic-Screening

Non-Relativistic

SM-Screening

Relativistic

Meissner-Mass

Static Vector PotentialWeak-GB-Mass

Hidden structure ????

Elementary Higgs: Elementary Higgs:

Trivial and Non-Trivial and Non-naturalnatural

Natural ScalarsNatural Scalars

Exact Super Symmetry:Exact Super Symmetry:

Fermions ↔ Bosons

Fermion’s custodial symmetry protects the Bosons

Observe: susy partners

Composite ScalarComposite Scalar:

Recall Superconductivity

Substructure resolved at scale ΛS

Observe: New Bound States

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.

Electroweak Symmetry Breaking

@

LHC

Electroweak Symmetry Breaking

SUSY

Extra Dim.

Technicolor

Curved Flat

Technicolor

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

Natural to use QCD-like dynamics.

Problems with the Old Models

• S-parameter: too large

• Large Flavor Changing Neutral Currents (FCNC)

• Limited knowledge of strong dynamics!

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

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…

Why the walking can help ?

QCD-Like

Near the conformal window

~

~

Critical Number of techniflavors

For fermions in the fundamental representation near conformal means:

The number of techndoublets is

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

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

The Model: The generalized S-Theory

Inspired by progress in

Strong Interactions

`t Hooft - Large N

Corrigan and Ramond `79

Larks

Kiritsis and Papavassiliou `90.

Ryttov and F.S. `05

Helpful for MC ???

Relation with Super Yang-Mills

A-typeA-typeS-typeS-type

SYMSYM

Armoni-Shifman-Veneziano

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

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

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

Nf=2 & N=2:

Minimal-Walking-Theory

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

S-parameter

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

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

Model versus EWPData

68% contour

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

Standard Hypercharge Assignment

150 GeV

4th Lepton Family

A natural LCH*

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

Phenomenology of a LCH

Associate Higgs production

Zerwekh 05

Spectrum

Techni-Mesons

Techni-Baryons Electric Charge

An Effective Theory

Some Scenarios

Dark Side of the 5th Force

NussinovBarr, Chivukula and Farhi

Technibaryon, DD

Universe Charge Neutrality.

Chemical Equilibrium

Taking care of the Sphaleron Processes

Gudnason, Kouvaris, F.S. ph -0603014

• 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

SUSY

TC

LHC

ED

Spectrum and Effective Theory I

Spectrum and Effective Theory II

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

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?