dynamical electroweak breaking @ lhcconsistency of the theory yw cms data 1 5 fb1, 3 5 fb1, 5 13...

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Francesco Sannino Composite Dynamics Vienna - November 25 - 2011

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Page 1: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

September 2011

Francesco Sannino

Composite Dynamics

CP3-DESY-Goettingen School 11-14 October 2011Vienna - November 25 - 2011

Page 2: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Francesco Sannino

Riddles

Page 3: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Atoms4%

Dark Matter22%

Dark Energy74%

Francesco Sannino

Riddles

Page 4: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Atoms4%

Dark Matter22%

Dark Energy74%

Francesco Sannino

Riddles

Page 5: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Atoms4%

Dark Matter22%

Dark Energy74%

Francesco Sannino

Riddles

Page 6: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Atoms4%

Dark Matter22%

Dark Energy74%

?Francesco Sannino

Riddles

Page 7: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Atoms4%

Dark Matter22%

Dark Energy74%

??Francesco Sannino

Riddles

Page 8: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Francesco Sannino

Standard Model

Page 9: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

SM

Francesco Sannino

Standard Model

Page 10: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

SM - GeometrySU(3)

SU(2)L

U(1)⊂SU(2)R

L-Leptons

R-Quarks

Weak GBGluons

R-Leptons

L-Quarks

Hyper - GBFrancesco Sannino

Page 11: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

SM - GeometrySU(3)

SU(2)L

U(1)⊂SU(2)R

Higgs

L-Leptons

R-Quarks

Weak GBGluons

R-Leptons

L-Quarks

Hyper - GB

Higgs Sector

Francesco Sannino

Page 12: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

SM - GeometrySU(3)

SU(2)L

U(1)⊂SU(2)R

<H>

Higgs

L-Leptons

R-Quarks

Weak GBGluons

R-Leptons

L-Quarks

Hyper - GB

Higgs Sector

Francesco Sannino

Page 13: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

SM - GeometrySU(3)

SU(2)L

U(1)⊂SU(2)R

U (1)Q

SU(3)

<H>

Higgs

L-Leptons

R-Quarks

Weak GBGluons

R-Leptons

L-Quarks

Hyper - GB

Higgs Sector

Francesco Sannino

Page 14: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

SM - GeometrySU(3)

SU(2)L

U(1)⊂SU(2)R

U (1)Q

SU(3)

<H>

Higgs

L-Leptons

R-Quarks

Weak GBGluons

R-Leptons

L-Quarks

Hyper - GB

Branish

Higgs Sector

Francesco Sannino

Page 15: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

O’ Higgs, where art thou!

© Francesco Sannino

Page 16: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

© Francesco Sannino

Page 17: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

MSSM Status

© Francesco Sannino

Page 18: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

© Francesco Sannino

MSUGRA/CMSSM = five parameters: the universal scalar mass m0, gaugino mass m1/2, the trilinear scalar coupling A0, tan β: the ratio of the VEV of the two Higgses the sign of the higgsino mass parameter μ.

ATLAS Experiment © 2011 CERN

Page 19: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

ATLAS Experiment © 2011 CERN

Page 20: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

What else has LHC not seen ?

© Francesco Sannino

Page 21: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

ATLAS Experiment © 2011 CERN

Page 22: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

What about Technicolor ?

© Francesco Sannino

Page 23: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Tevatron

Consistency of the theory

YW

CMS Data �1⇥5 fb�1, 3 ⇥5 fb�1, 5 ⇥13 TeV, 100 fb�1, 3 ⇥13 TeV, 100 fb�1, 5 ⇥

0.5 1.0 1.5 2.0 2.5

2

4

6

8

10

12

MA ⇤TeV⌅

g⇤Walking

Running

Andersen, Hapola, Sannino 11Belyaev, Foad, Frandsen, Jarvinen, Pukhov, Sannino 08

Page 24: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Tevatron

Consistency of the theory

YW

CMS Data �1⇥5 fb�1, 3 ⇥5 fb�1, 5 ⇥13 TeV, 100 fb�1, 3 ⇥13 TeV, 100 fb�1, 5 ⇥

0.5 1.0 1.5 2.0 2.5

2

4

6

8

10

12

MA ⇤TeV⌅

g⇤Walking

Running

Andersen, Hapola, Sannino 11Belyaev, Foad, Frandsen, Jarvinen, Pukhov, Sannino 08

Much unexplored !

Page 25: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Tevatron

Consistency of the theory

YW

CMS Data �1⇥5 fb�1, 3 ⇥5 fb�1, 5 ⇥13 TeV, 100 fb�1, 3 ⇥13 TeV, 100 fb�1, 5 ⇥

0.5 1.0 1.5 2.0 2.5

2

4

6

8

10

12

MA ⇤TeV⌅

g⇤Walking

Running

Andersen, Hapola, Sannino 11Belyaev, Foad, Frandsen, Jarvinen, Pukhov, Sannino 08

Much unexplored !

Page 26: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Technicolor - Geometry

SU(3)

SU(2)L

U(1)⊂SU(2)R

Francesco Sannino

Page 27: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Technicolor - Geometry

SU(3)

SU(2)L

U(1)⊂SU(2)R

TC

R-TQuarks

L-TQuarks

Technicolor

Francesco Sannino

Page 28: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Technicolor - Geometry

SU(3)

SU(2)L

U(1)⊂SU(2)R

TC

< Q Q>_

R-TQuarks

L-TQuarks

Technicolor

Francesco Sannino

Page 29: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Technicolor - Geometry

U (1)Q

SU(3)SU(3)

SU(2)L

U(1)⊂SU(2)R

TC

< Q Q>_

R-TQuarks

L-TQuarks

Technicolor

Francesco Sannino

Page 30: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Dynamical EW Breaking

Francesco Sannino

Page 31: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

L(H)⇤ �14F aµ⇥F a

µ⇥ + i Q̄�µDµQ + · · ·

Dynamical EW Breaking

Francesco Sannino

Page 32: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Dots are partially fixed by Anomalies as well as other principles

L(H)⇤ �14F aµ⇥F a

µ⇥ + i Q̄�µDµQ + · · ·

Dynamical EW Breaking

Francesco Sannino

Page 33: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Dots are partially fixed by Anomalies as well as other principles

L(H)⇤ �14F aµ⇥F a

µ⇥ + i Q̄�µDµQ + · · ·

· · · ⇥ L(New SM Fermions)

Dynamical EW Breaking

Francesco Sannino

Page 34: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

-0.2 0.0 0.2 0.4-0.1

0.0

0.1

0.2

0.3

0.4

0.5

S

T

SU(3) + 1 Fund. Doublet Weinberg, Susskind1 TeV

Large & Positive S from QCD-like Technicolor

Need novel dynamics

Page 35: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

SM Fermion Masses

Francesco Sannino

Page 36: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

L̄ · HeR ⇥ L̄Q̄Q

�2ETC

eR

Extending Technicolor

Francesco Sannino

Page 37: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Different Approaches

Francesco Sannino

Page 38: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Scalar-less New Gauge Interactions (Extended TC)

Different Approaches

Francesco Sannino

Page 39: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Scalar-less New Gauge Interactions (Extended TC)

Marry SUSY and Technicolor

Different Approaches

Francesco Sannino

Page 40: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Scalar-less New Gauge Interactions (Extended TC)

Marry SUSY and Technicolor

Add New Scalars in the Flavor Sector

Different Approaches

Francesco Sannino

Page 41: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Scalar-less New Gauge Interactions (Extended TC)

Marry SUSY and Technicolor

Add New Scalars in the Flavor Sector

.....

Different Approaches

Francesco Sannino

Page 42: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Naive Extended Technicolor

Eichten & Lane 80

Francesco Sannino

Page 43: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Naive Extended Technicolor

Eichten & Lane 80

Recent investigationsRyttov & Shrock 10

Francesco Sannino

Page 44: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Naive Extended Technicolor

Eichten & Lane 80

Recent investigationsRyttov & Shrock 10

Francesco Sannino

Page 45: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

PNGMasses

Naive Extended Technicolor

Eichten & Lane 80

Recent investigationsRyttov & Shrock 10

Francesco Sannino

Page 46: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

PNGMasses

SM-FermionMasses

Naive Extended Technicolor

Eichten & Lane 80

Recent investigationsRyttov & Shrock 10

Francesco Sannino

Page 47: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

PNGMasses

SM-FermionMasses

FCNCOperators

Naive Extended Technicolor

Eichten & Lane 80

Recent investigationsRyttov & Shrock 10

Francesco Sannino

Page 48: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

PNGMasses

SM-FermionMasses

FCNCOperators

Naive Extended Technicolor

Modifies TC dynamics

Eichten & Lane 80

Recent investigationsRyttov & Shrock 10

Francesco Sannino

Page 49: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

PNGMasses

SM-FermionMasses

FCNCOperators

Naive Extended Technicolor

Modifies TC dynamics

Eichten & Lane 80

Recent investigationsRyttov & Shrock 10

Francesco Sannino

Antola, Di Chira, Sannino, Tuominen 10,11

Page 50: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Francesco Sannino

Page 51: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

mf �g2

ETC

�2ETC

< Q̄Q >ETC⇤ETC

Francesco Sannino

Page 52: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

mf �g2

ETC

�2ETC

< Q̄Q >ETC⇤ETC

⇤TC Electroweak breaks

Francesco Sannino

Page 53: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

mf �g2

ETC

�2ETC

< Q̄Q >ETC⇤ETC

⇤TC Electroweak breaks

< Q̄Q >ETC ⇥< Q̄Q >TC � �3TC

Francesco Sannino

Page 54: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

mf �g2

ETC

�2ETC

< Q̄Q >ETC⇤ETC

⇤TC

mf �g2

ETC

�2ETC

< Q̄Q >ETC ⇥ mTop

Electroweak breaks

< Q̄Q >ETC ⇥< Q̄Q >TC � �3TC

Francesco Sannino

Page 55: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Need to go beyond QCD

Francesco Sannino

Page 56: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Near Conformal

Francesco Sannino

Page 57: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Near Conformal

UVIR

Francesco Sannino

Page 58: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Near Conformal

UVIR

IR Conformal behavior

Francesco Sannino

Page 59: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Near Conformal

UVIR

IR Conformal behavior

Francesco Sannino

Page 60: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Why walking helps?

Francesco Sannino

Page 61: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

QCD-Like

~

Why walking helps?

Francesco Sannino

Page 62: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

QCD-Like

Near the conformal window

~

~

Why walking helps?

Francesco Sannino

Page 63: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

QCD-Like

Near the conformal window

~

~

Why walking helps?

Francesco Sannino

Page 64: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

mf �g2

ETC

�2ETC

< Q̄Q >ETC=g2

ETC

�2ETC

��ETC

�TC

⇥⇥m(��)

< Q̄Q >TC

If large anomalous dimension, around ⇥m(�⇤) ⇠ 1.7

Francesco Sannino

Page 65: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

mf �g2

ETC

�2ETC

< Q̄Q >ETC=g2

ETC

�2ETC

��ETC

�TC

⇥⇥m(��)

< Q̄Q >TC

If large anomalous dimension, around ⇥m(�⇤) ⇠ 1.7

Francesco Sannino

Page 66: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

mf �g2

ETC

�2ETC

< Q̄Q >ETC=g2

ETC

�2ETC

��ETC

�TC

⇥⇥m(��)

< Q̄Q >TC

If large anomalous dimension, around ⇥m(�⇤) ⇠ 1.7

Fermion Mass Enhancement & FCNC decoupling

Francesco Sannino

Page 67: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Ingredients

Francesco Sannino

Page 68: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6
Page 69: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

๏ Understand Phase Diagram of gauge theories

Page 70: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

๏ Understand Phase Diagram of gauge theories

๏ Walking: Is it really phenomenologically viable?

Page 71: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

๏ Understand Phase Diagram of gauge theories

๏ Walking: Is it really phenomenologically viable?

๏ Need a working example of ETC

Page 72: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Phase diagram

Francesco Sannino

Page 73: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Knobs

Francesco Sannino

Page 74: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauge Group, i.e. SU, SO, SP

Knobs

Francesco Sannino

Page 75: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauge Group, i.e. SU, SO, SP

Matter Representation

Knobs

Francesco Sannino

Page 76: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauge Group, i.e. SU, SO, SP

Matter Representation

# of Flavors per Representation

Knobs

Francesco Sannino

Page 77: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauge Group, i.e. SU, SO, SP

Matter Representation

# of Flavors per Representation

Knobs

Nf

Francesco Sannino

Page 78: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauge Group, i.e. SU, SO, SP

Matter Representation

# of Flavors per Representation

Knobs

NfQCD

Francesco Sannino

Page 79: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauge Group, i.e. SU, SO, SP

Matter Representation

# of Flavors per Representation

Knobs

NfQCD IR Conformal

Francesco Sannino

Page 80: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauge Group, i.e. SU, SO, SP

Matter Representation

# of Flavors per Representation

Knobs

NfQCD IR Conformal Infrared free

Francesco Sannino

Page 81: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauge Group, i.e. SU, SO, SP

Matter Representation

# of Flavors per Representation

Knobs

NfQCD IR Conformal Infrared free

Francesco Sannino

Page 82: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauge Group, i.e. SU, SO, SP

Matter Representation

# of Flavors per Representation

Knobs

NfQCD IR Conformal Infrared free

Francesco Sannino

?

Page 83: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

A novel phase @ large Nf

NfQCD IR Conformal

Francesco Sannino

Pica & Sannino 10

Page 84: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Interesting structure at large Nf

A novel phase @ large Nf

NfQCD IR Conformal

Francesco Sannino

Pica & Sannino 10

Page 85: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Interesting structure at large Nf

A novel phase @ large Nf

NfQCD IR Conformal

Francesco Sannino

Entire series at large Nf is known

Pica & Sannino 10

Page 86: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

α

Energy

Interesting structure at large Nf

A novel phase @ large Nf

NfQCD IR Conformal Asymp. Safe

Francesco Sannino

Entire series at large Nf is known

Pica & Sannino 10

Page 87: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

α

Energy

Interesting structure at large Nf

A novel phase @ large Nf

NfQCD IR Conformal Asymp. Safe

Francesco Sannino

Entire series at large Nf is known

Pica & Sannino 10

�UV =3⇥

TFNf

Page 88: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Universal Picture

Francesco Sannino

Page 89: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Fund

2A

2S

Adj

Ladder

Ryttov & Sannino 07

SU(N) Phase Diagram

Dietrich & Sannino 07

Sannino & Tuominen 04

Pica & Sannino 10

Francesco Sannino

Page 90: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Fund

2A

2S

Adj

Ladder

Ryttov & Sannino 07

SU(N) Phase Diagram

Dietrich & Sannino 07

Sannino & Tuominen 04

Pica & Sannino 10

Francesco Sannino

Page 91: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Fund

2A

2S

Adj

Ladder

Ryttov & Sannino 07

SU(N) Phase Diagram

Dietrich & Sannino 07

Sannino & Tuominen 04

Pica & Sannino 10

Francesco Sannino

Page 92: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Fund

2A

2S

Adj

Ladder

Ryttov & Sannino 07

SU(N) Phase Diagram

Dietrich & Sannino 07

Sannino & Tuominen 04

Pica & Sannino 10

Francesco Sannino

Very interesitng

Page 93: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Lattice SU(N) Phase Diagram

Fund

2A

2SAdj

�SD ' 1�PS = 1

�PS = 0.5

Page 94: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

iWalk

© Francesco Sannino

Page 95: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

iWalk = ideal Walking

© Francesco Sannino

Dietrich Sannino 06Fukano & Sannino 10

Page 96: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

iWalk = ideal Walking

Walking is fine tuned

© Francesco Sannino

Dietrich Sannino 06Fukano & Sannino 10

Page 97: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

iWalk = ideal Walking

Walking is fine tuned

Anomalous dimensions may be small

© Francesco Sannino

Dietrich Sannino 06Fukano & Sannino 10

Page 98: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

iWalkFukano & Sannino 10

© Francesco Sannino

Appelquist, Soldate, Takeuchi and Wijewardhana, 88Kondo, Mino, Yamawaki 89Takeuchi 96Yamawaki, Kurachi and Shrock 08

Page 99: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

iWalkFukano & Sannino 10

L(H)⇤ �14F aµ⇥F a

µ⇥ + i Q̄�µDµQ + · · ·

© Francesco Sannino

Appelquist, Soldate, Takeuchi and Wijewardhana, 88Kondo, Mino, Yamawaki 89Takeuchi 96Yamawaki, Kurachi and Shrock 08

Page 100: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

iWalkFukano & Sannino 10

L(H)⇤ �14F aµ⇥F a

µ⇥ + i Q̄�µDµQ + · · ·

© Francesco Sannino

Appelquist, Soldate, Takeuchi and Wijewardhana, 88Kondo, Mino, Yamawaki 89Takeuchi 96Yamawaki, Kurachi and Shrock 08

Page 101: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

iWalkFukano & Sannino 10

L(H)⇤ �14F aµ⇥F a

µ⇥ + i Q̄�µDµQ + · · ·

© Francesco Sannino

Appelquist, Soldate, Takeuchi and Wijewardhana, 88Kondo, Mino, Yamawaki 89Takeuchi 96Yamawaki, Kurachi and Shrock 08

Page 102: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauged Nambu Jona-Lasinio

2 3 4 5 6 7 8 9 100

5

10

15

20

N

Nf

Fukano & Sannino 10� ' 1.73

Fukano & Sannino 10

© Francesco Sannino

Page 103: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauged Nambu Jona-Lasinio

As if the number of flavors is continuous

2 3 4 5 6 7 8 9 100

5

10

15

20

N

Nf

Fukano & Sannino 10� ' 1.73

Fukano & Sannino 10

© Francesco Sannino

Page 104: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauged Nambu Jona-Lasinio

As if the number of flavors is continuous

Anomalous dimensions increase

2 3 4 5 6 7 8 9 100

5

10

15

20

N

Nf

Fukano & Sannino 10� ' 1.73

Fukano & Sannino 10

© Francesco Sannino

Page 105: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauged Nambu Jona-Lasinio

As if the number of flavors is continuous

Anomalous dimensions increase

2 3 4 5 6 7 8 9 100

5

10

15

20

N

Nf

Fukano & Sannino 10� ' 1.73

Phenomenologically viable

Fukano & Sannino 10

© Francesco Sannino

Page 106: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Gauged Nambu Jona-Lasinio

As if the number of flavors is continuous

Anomalous dimensions increase

2 3 4 5 6 7 8 9 100

5

10

15

20

N

Nf

Fukano & Sannino 10� ' 1.73

Phenomenologically viable

Being tested!

Fukano & Sannino 10

© Francesco Sannino

Page 107: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Minimal Working TC

UD

Francesco Sannino

Page 108: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Minimal Working TC

UD

Minimal WT

SU(2)TCNE

Sannino & Tuominen 04

Dietrich, Sannino, Tuominen 05

Frandsen, Masina, Sannino 09

Francesco Sannino

Page 109: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Minimal Working TC

UD

Minimal WT

Next to MWT

SU(2)TC

SU(3)TC

NE

Sannino & Tuominen 04

Dietrich, Sannino, Tuominen 05

Dietrich, Sannino, Tuominen 05

Sannino, Tuominen 04UD

Frandsen, Masina, Sannino 09

Francesco Sannino

Page 110: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Minimal Working TC

UD

Minimal WT

Next to MWT

Orthogonal

SU(2)TC

SU(3)TC

SO(4)TC

NE

Frandsen, Sannino 09

Sannino & Tuominen 04

Dietrich, Sannino, Tuominen 05

Dietrich, Sannino, Tuominen 05

Sannino, Tuominen 04UD

UD

Frandsen, Masina, Sannino 09

Francesco Sannino

Page 111: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Minimal Working TC

UD

Minimal WT

Next to MWT

Orthogonal

SU(2)TC

SU(3)TC

SO(4)TC

Ultra MT

SU(2)TC

NE

Frandsen, Sannino 09

Ryttov & Sannino 08

Sannino & Tuominen 04

Dietrich, Sannino, Tuominen 05

Dietrich, Sannino, Tuominen 05

Sannino, Tuominen 04UD

UD

UD

Frandsen, Masina, Sannino 09

Francesco Sannino

Vanilla TC

Page 112: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Minimal Walking Technicolor

Page 113: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

SU(3)

SU(2)

U(1)

F.S. + Tuominen 04Dietrich, F.S., Tuominen 05

Page 114: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Extra Electron SU(3)

SU(2)

U(1)

U

D

Gt-up

t-down

t-glue SU(2)

NExtraNeutrino

U and D: Adj of SU(2)

F.S. + Tuominen 04Dietrich, F.S., Tuominen 05

Page 115: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

S beyond TC...

Page 116: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

S = S(W )TC + SNS

S beyond TC...

Page 117: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

S = S(W )TC + SNS

S beyond TC...

Page 118: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

S = S(W )TC + SNS

Offset the first term

S beyond TC...

Page 119: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

New Leptons & Precision Data

1 TeV

117 GeV

300 GeV

Exotic Leptonic hypercharge Y=-3/2 Standard Model Leptonic hypercharge

Page 120: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

MWT Features

Page 121: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

MWT Features

๏ The most economical WT theory

Page 122: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

MWT Features

๏ The most economical WT theory

๏ Compatible with precision measurements

Page 123: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

MWT Features

๏ The most economical WT theory

๏ Compatible with precision measurements

๏ Possible DM candidates

Page 124: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

MWT Features

๏ The most economical WT theory

๏ Compatible with precision measurements

๏ Possible DM candidates

๏ Under investigation on the Lattice

Page 125: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

L(Composites) + L(Mixing with SM) + L(New Leptons) + L(SM�Higgs)

MWT Effective Lagrangian

Foadi, Frandsen, Ryttov & F.S. 07

Page 126: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Composite Higgs H

Composite Axial - Vector States

L(Composites) + L(Mixing with SM) + L(New Leptons) + L(SM�Higgs)

R1,2

MWT Effective Lagrangian

Foadi, Frandsen, Ryttov & F.S. 07

Page 127: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Composite Higgs H

Composite Axial - Vector States

L(Composites) + L(Mixing with SM) + L(New Leptons) + L(SM�Higgs)

R1,2

MWT Effective Lagrangian

Heavy Electron

2 Heavy Majoranas N1 N2

Frandsen, Masina, Sannino 09

Hapola, Masina, Sannino 11 Foadi, Frandsen, Ryttov & F.S. 07

Page 128: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Tevatron

Consistency of the theory

YW

CMS Data �1⇥5 fb�1, 3 ⇥5 fb�1, 5 ⇥13 TeV, 100 fb�1, 3 ⇥13 TeV, 100 fb�1, 5 ⇥

0.5 1.0 1.5 2.0 2.5

2

4

6

8

10

12

MA ⇤TeV⌅

g⇤

Walking

Running

Constraining MWT

Page 129: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Tevatron

Consistency of the theory

YW

CMS Data �1⇥5 fb�1, 3 ⇥5 fb�1, 5 ⇥13 TeV, 100 fb�1, 3 ⇥13 TeV, 100 fb�1, 5 ⇥

0.5 1.0 1.5 2.0 2.5

2

4

6

8

10

12

MA ⇤TeV⌅

g⇤

Walking

Running

Constraining MWT

Andersen, Hapola, Sannino 11Belyaev, Foad, Frandsen, Jarvinen, Pukhov, Sannino 08

Page 130: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Dark Matter

Francesco Sannino

Page 131: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Atoms4%

Dark Matter22%Dark Energy

74%

Dark Matter

Francesco Sannino

Page 132: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Atoms4%

Dark Matter22%Dark Energy

74%

Dark Matter

�DM

�B� 5

Francesco Sannino

Page 133: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

What makes DM?

Atoms4%

Dark Matter22%

Francesco Sannino

Page 134: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

What makes DM?

Atoms4%

Dark Matter22%

?Francesco Sannino

Page 135: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

What makes DM?

Atoms4%

Dark Matter22%

?Francesco Sannino

???

DM Particle

Page 136: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

What makes DM?

Atoms4%

Dark Matter22%

?Francesco Sannino

???

DM Particle

Elementary

Page 137: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

What makes DM?

Atoms4%

Dark Matter22%

?Francesco Sannino

Composite

???

DM Particle

Elementary

Page 138: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

What makes DM?

Atoms4%

Dark Matter22%

?Francesco Sannino

Composite

???

DM Particle

Elementary

Oversimplification

Page 139: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

�B DM asymmetry

Page 140: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

�B DM asymmetry

A particle similar to the nucleon

Page 141: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

�B DM asymmetry

A particle similar to the nucleon

Electrically neutral

Page 142: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

�B DM asymmetry

A particle similar to the nucleon

Electrically neutral

At most EW-type cross sections

Page 143: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

�B DM asymmetry

A particle similar to the nucleon

Electrically neutral

At most EW-type cross sections

Great if connected to EW (Observable at LHC)

Page 144: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Composite Dark Matter (Un)TC Interact. Massive Particle (u)TIMP

Page 145: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Composite Dark Matter

TIMPs Masses Annih. Asymm Symm Models

TC-Baryon (1 - 3) TeV - X -Complex-RepTraditional TC

TC-PGB 5 GeV - .5 TeV X X X(Pseudo)-Real

(UMT, MWT, OT)

Unbaryon (1 - 10) GeV X X X Techni-unparticle

(Un)TC Interact. Massive Particle (u)TIMP

Page 146: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Composite Dark Matter

TIMPs Masses Annih. Asymm Symm Models

TC-Baryon (1 - 3) TeV - X -Complex-RepTraditional TC

TC-PGB 5 GeV - .5 TeV X X X(Pseudo)-Real

(UMT, MWT, OT)

Unbaryon (1 - 10) GeV X X X Techni-unparticle

(Un)TC Interact. Massive Particle (u)TIMP

Page 147: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Composite Dark Matter

TIMPs Masses Annih. Asymm Symm Models

TC-Baryon (1 - 3) TeV - X -Complex-RepTraditional TC

TC-PGB 5 GeV - .5 TeV X X X(Pseudo)-Real

(UMT, MWT, OT)

Unbaryon (1 - 10) GeV X X X Techni-unparticle

(Un)TC Interact. Massive Particle (u)TIMP

Page 148: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Composite Dark Matter

TIMPs Masses Annih. Asymm Symm Models

TC-Baryon (1 - 3) TeV - X -Complex-RepTraditional TC

TC-PGB 5 GeV - .5 TeV X X X(Pseudo)-Real

(UMT, MWT, OT)

Unbaryon (1 - 10) GeV X X X Techni-unparticle

(Un)TC Interact. Massive Particle (u)TIMP

Page 149: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Composite Dark Matter

TIMPs Masses Annih. Asymm Symm Models

TC-Baryon (1 - 3) TeV - X -Complex-RepTraditional TC

TC-PGB 5 GeV - .5 TeV X X X(Pseudo)-Real

(UMT, MWT, OT)

Unbaryon (1 - 10) GeV X X X Techni-unparticle

(Un)TC Interact. Massive Particle (u)TIMP

TC-PGB Ryttov - Sannino 08Frandsen & Sannino. 09

Gudnason - Kouvaris - Sannino. 06

TC-Baryon

Nussinov, 86Barr - Chivukula - Farhi 90Sarkar 96Gudnason - Kouvaris - F.S. 06

Nardi, Sannino., Strumia, 08.Foadi, Frandsen, Sannino 09

Sannino, 10Related Kouvaris 06,07,10Kainulainen, Virkajarvi, Tuominen 06,09,10

Belyaev, Frandsen, Sannino, Sarkar 10

Mixed TIMP DM

Unbaryon Sannino, Zwicky 09Frandsen, Sarkar, 10

D.B. Kaplan 92

Page 150: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

DM and GUTs

Francesco Sannino

Page 151: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

�TB

�B=

TB

B

mTB

mp� O(1)

DM and GUTs

Francesco Sannino

Page 152: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

�TB

�B=

TB

B

mTB

mp� O(1)

DM and GUTs

TB

B� O(1)

Light

mTB ⇠ 5 GeV

Francesco Sannino

Page 153: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

�TB

�B=

TB

B

mTB

mp� O(1)

DM and GUTs

TB

B� O(1)

Light

mTB ⇠ 5 GeV

TB

B⇡ exp

h�mTB

T ⇤

i

Heavy

mTB ⇡ (1� 3) TeV

Francesco Sannino

Page 154: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

�TB

�B=

TB

B

mTB

mp� O(1)

DM and GUTs

� ⇠ M4GUT

m5TB

⇠ 1026sec

GUTs

� ⇠ M4GUT

m5TB

⇠ 3⇥ 1037sec

Nardi, FS, Strumia, 08.

Gudnason, Ryttov, FS 06

TB

B� O(1)

Light

mTB ⇠ 5 GeV

TB

B⇡ exp

h�mTB

T ⇤

i

Heavy

mTB ⇡ (1� 3) TeV

Francesco Sannino

Page 155: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Puzzle

7.5 8.0 8.5 9.010-42

10-41

10-40

10-39

Mf in GeV

spincm

2 CoGeNT

DAMA

Xenon 100Xenon 10

CDMS

Page 156: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Higgs

Del Nobile, Kouvaris, Sannino 11

DarkMatter

DarkMatter

+ �

Quantum Mechanics

Page 157: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Interfering Composite ADM

CoGeNT and DAMA Del Nobile, Kouvaris, Sannino 11

7.5 8.0 8.5 9.0

10-38

10-37

Mf in GeV

spincm

2 CoGeNT

DAMA

Xenon 100Xenon 10CDMS

Page 158: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Interfering Composite ADM

CoGeNT and DAMA Del Nobile, Kouvaris, Sannino 11

7.5 8.0 8.5 9.0

10-38

10-37

Mf in GeV

spincm

2 CoGeNT

DAMA

Xenon 100Xenon 10CDMS

Chang et al. 2010, Feng et al, 2011, Frandsen et al. 2011

Page 159: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

Conclusions

Page 160: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

๏ DEWSB can naturally occur at the LHC

Conclusions

Page 161: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

๏ DEWSB can naturally occur at the LHC

๏ Phase Diagram of strongly interacting theories

Conclusions

Page 162: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

๏ DEWSB can naturally occur at the LHC

๏ Phase Diagram of strongly interacting theories

๏ Minimal models of technicolor

Conclusions

Page 163: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

๏ DEWSB can naturally occur at the LHC

๏ Phase Diagram of strongly interacting theories

๏ Minimal models of technicolor

๏ Composite Dark Matter

Conclusions

Page 164: Dynamical Electroweak Breaking @ LHCConsistency of the theory YW CMS Data 1 5 fb1, 3 5 fb1, 5 13 TeV, 100 fb1, 3 13 TeV, 100 fb1, 5 0.5 1.0 1.5 2.0 2.5 2 4 6

๏ DEWSB can naturally occur at the LHC

๏ Phase Diagram of strongly interacting theories

๏ Minimal models of technicolor

๏ Composite Dark Matter

๏ Composite inflation... another time

Conclusions