50
何何何 何何何 清清清清 清清清清 LHC: Seeking the Origin of LHC: Seeking the Origin of Symmetry Breaking and Mass Symmetry Breaking and Mass LHC: LHC: 何何何何何何何何何何何何 何何何何何何何何何何何何 Nanchang, April 17-19, 2010.

何红建 清华大学

Embed Size (px)

DESCRIPTION

LHC: Seeking the Origin of Symmetry Breaking and Mass LHC: 探索对称性破缺与质量起源. 何红建 清华大学. Nanchang, April 17-19, 2010. LHC: this not the end of the beginning --. It is beginning of the new start !. L. H. C. LHC Runs: 7 TeV… 10 TeV… 14 TeV……. What discovery expected at LHC ? - PowerPoint PPT Presentation

Citation preview

Page 1: 何红建 清华大学

何红建何红建清华大学清华大学

LHC: Seeking the Origin of LHC: Seeking the Origin of Symmetry Breaking and MassSymmetry Breaking and Mass

LHC: LHC: 探索对称性破缺与质量起源探索对称性破缺与质量起源

Nanchang, April 17-19, 2010.

Page 2: 何红建 清华大学
Page 3: 何红建 清华大学

LHC: this not the end of the beginning --

L H C

It is beginning of the new start !

Page 4: 何红建 清华大学

What discovery expected at LHC ?What discovery expected at LHC ?

What should What should WeWe dodo for it ? for it ?

LHC Runs: 7TeV…10TeV…14TeV……

Page 5: 何红建 清华大学

All Matter(Spin-1/2)+Forces(Spin-1) are discovered in SM!The only Missing Particle: Higgs Boson H0 (Spin-0).Higgs Boson gives Masses to All Particles except γ, gluons.

Page 6: 何红建 清华大学

All SM Particles: All SM Particles: Area of circle Area of circle ∝∝ Particle-Mass Particle-Mass Only Top, W/Z and Only Top, W/Z and HiggsHiggs stand out ! stand out !

Page 7: 何红建 清华大学

All spin-1/2 matter particles have Masses ∝∝ Arbitrary Yukawa Couplings:

??

( Mw = g v/2 )

Page 8: 何红建 清华大学

SM: (Un)Naturalness of Matter MassesSM: (Un)Naturalness of Matter Masses

•Only Top & Neutrino masses are Natural

(adding Right-handed Neutrinos):

•But, Why All Other Yukawa’s so tiny ?? e.g.,

Page 9: 何红建 清华大学

It is often said that It is often said that LHCLHC is just to find is just to find a light fundamental Higgs Bosona light fundamental Higgs Boson..

BUT, this is a quite misleading statement BUT, this is a quite misleading statement --

1. 1. Higgs Boson may be Higgs Boson may be heavyheavy. .

2. 2. Higgs may be Higgs may be more than one more than one andand charged charged..

3. 3. Higgs Boson may be Higgs Boson may be compositecomposite. .

4. 4. Higgs Boson may Higgs Boson may Not exit Not exit at all.at all.

5. 5. Smoking-Gun Signals Smoking-Gun Signals other than Higgsother than Higgs..

Page 10: 何红建 清华大学

10

The two best measurements of

sin2W do not agree :

NO compelling evidence for

Light Higgs Boson even in SM !

★ Possibility of Heavy Higgs or No Higgs is fully open !

See: Gian Giudice (CERN), talk at Tsinghua on 3-28-2010

Page 11: 何红建 清华大学

Heavy Higgs vs Precision Data:Heavy Higgs vs Precision Data: No Problem !No Problem !

HJH etal, TopSeesaw Composite Higgs mH ≈ 400-500GeV

Top Seesaw Model

Page 12: 何红建 清华大学

““Natural” SUSY requires heavier Higgs too !Natural” SUSY requires heavier Higgs too !

MSSM is alreadyFine-tuned !

Extended SUSYs give:

Barbieri et al, 1004.2256

Page 13: 何红建 清华大学

Fine-Tuning Problem ? Fine-Tuning Problem ?

● Radiative Corrections to Higgs Mass:

● Degree of Fine-Tuning (DFT):

Page 14: 何红建 清华大学

Fine-Tuning Fine-Tuning is ais a Technical ProblemTechnical Problem ! !

Not strong enough for LHC (ILC) !Not strong enough for LHC (ILC) !

3TeV

6.5TeV

0.05

10TeV

0.01

7TeV

14.5TeV

Page 15: 何红建 清华大学

Mysteries of Mass Origin: Mysteries of Mass Origin: What can LHC probe ? What can LHC probe ?

GeV

ν10-2 eV

Origin of Electroweak Symmetry Breaking: -- Why are (W, Z) Massive but photon Massless ?

Does t-Quark conspire Electroweak Symmetry Breaking: -- Why is t-Quark Mass so Close to W/Z Masses ? Why is Neutrino Mass so tiny ? → Seesaw Mechanism !

Page 16: 何红建 清华大学

Origin of Electroweak Symmetry Breaking:Origin of Electroweak Symmetry Breaking: Why Why Higgs Boson (light or heavy)Higgs Boson (light or heavy) at all ?!? at all ?!?

Real Physics ProblemReal Physics Problem withwith Electroweak Symmetry BreakingElectroweak Symmetry Breaking isis

Unitarity ViolationUnitarity Violation

inin High Energy ScatteringHigh Energy Scattering !!!!!!!!!!

Page 17: 何红建 清华大学

Unitarity of WUnitarity of WLLWWLL → W → WLLWWLL: :

Electroweak Symmetry Breaking ScaleElectroweak Symmetry Breaking Scale

Much Stronger & More Robust than Fine-tuning bound!

No Way to Escape this Physics Bound !!!

Page 18: 何红建 清华大学

0.7

Page 19: 何红建 清华大学

A A New Way New Way to to RestoreRestore UnitarityUnitarity::

Higgsless TheoryHiggsless Theory !!!!!!

Crucial Observation:

New Spin-1 Gauge Bosons can Replace Spin-0 Higgs to Restore Unitarity !!!

Chivukula,Dicus,He, 2001: New Gauge Bosons from 5d-KKChivukula,He, 2002: New Gauge Bosons from 4d-Deconstructionand 19 series papers in 2003-2009

Page 20: 何红建 清华大学
Page 21: 何红建 清华大学
Page 22: 何红建 清华大学
Page 23: 何红建 清华大学

LHC Signals for Higgsless W1 Boson: pp→W1 Z→WZZ→jj+4Leptons pp→jjWZ (including WZ─W1*→WZ→3l+nu)

HJH, YPK,YHQ, BZ & MSU arXiv:0708.2588

Page 24: 何红建 清华大学

LHC Sensitivity for WLHC Sensitivity for W11

in WZZ & jjWZ Channels:in WZZ & jjWZ Channels:

HJH, YPK, YHQ, BZ & MSU

Page 25: 何红建 清华大学

Does top-Quark Conspire Electroweak Symmetry Breaking ??

Why is t-Quark Mass

so Close to W/Z Masses ?

Page 26: 何红建 清华大学

50 Years Ago

Ni60

Lee and Yang, 1956

Parity

Page 27: 何红建 清华大学

We reveal the Intrinsic Connection between Spontaneous Parity Violation (SPV) and Electroweak Symmetry Breaking (EWSB)

SPV Scale is tied to TeV Scale

SPV Induces EWSB (W,Z Masses) as Uniquely fixed by Top-quark Mass = 174 GeV

Page 28: 何红建 清华大学

Predictions:Predictions: A Sample Higgs Spectrum A Sample Higgs Spectrum

E.g.

Page 29: 何红建 清华大学

LHC Discovery: LHC Discovery: Luminosity vs Higgs MassLuminosity vs Higgs Mass

Page 30: 何红建 清华大学

Signals at the LHCSignals at the LHC:: andand

pp (gb) → t H+ → t t b.pp → WR → bbW

Page 31: 何红建 清华大学

Scales of Fermion Mass GenerationScales of Fermion Mass Generation

New Physics that LHC canNot do ?New Physics that LHC canNot do ?

Page 32: 何红建 清华大学

Exciting Future: After LHC !!!

Page 33: 何红建 清华大学

New Physics that LHC New Physics that LHC cannotcannot do: do: Neutrino Neutrino Mixing,Mixing, CP-Violation, Matter-Antimatter CP-Violation, Matter-Antimatter Asymmetry…Asymmetry…

Page 34: 何红建 清华大学

Daya Bay’s Daya Bay’s Physics PotentialPhysics Potential on on θ13 isis Non-trivial Non-trivial to justify:to justify:

Page 35: 何红建 清华大学

Our Theory Prediction Our Theory Prediction givesgivesstrongest support strongest support forfor Daya BayDaya Bay !!! !!!

Ge, He, Yin, JCAP(2010), 1001.0940Ge, He, Yin, JCAP(2010), 1001.0940

Page 36: 何红建 清华大学

KeV TeV 1019 GeV

Nature may be more complicated and more interesting than we naively thouhght !!

Many New Scales ?Many New Forces ?Is Gravity Emergent?Is M_Planck fundamental?

Page 37: 何红建 清华大学

2010 ─ 2030

Keep Keep Your MindYour Mind Fully Open Fully Open !!!!!!

Page 38: 何红建 清华大学

Thank You !

Page 39: 何红建 清华大学

Backup SlidesBackup Slides

Page 40: 何红建 清华大学
Page 41: 何红建 清华大学

4 Fundamental Forces 4 Fundamental Forces evolve back withevolve back withTime/Temperature(Energy):UnificationTime/Temperature(Energy):Unification??

Page 42: 何红建 清华大学

Hierarchy/Fine-Tuning Problem ?Hierarchy/Fine-Tuning Problem ?

→→ Not strong enough !Not strong enough !

Unification ?Unification ?

→→ Many possible realizations !Many possible realizations !

Light Higgs ?Light Higgs ?

→→ Not enforced by data ! Not enforced by data ! Then, Then,

WHAT best justifies TeV Scale?WHAT best justifies TeV Scale? … …

New Physics at New Physics at TeVTeV Scale ?Scale ?

Page 43: 何红建 清华大学
Page 44: 何红建 清华大学

Fine-Tuning Problem ?Fine-Tuning Problem ?

SM Higgs Mass 1-Loop Quadratical Divergence:

Quadratical Divergence vanishes if

→No Fine-Tuning for MH around 300GeV !

Page 45: 何红建 清华大学

SM Higgs Potential runs intomore seriousVacuum Energy Problemeven at TREE-Level: (eg, S.Weinberg,

1989)

<ρ> = Vmin – λv4/4

= Vmin - O(100GeV)4 == (2∙10-3eV)4

→ 55 Orders of Magnitude Fine-tuning !

Soft Breaking SUSY faces the same problem!

So, WHY do we care 1% Tuning at 1-Loop?!

Neutrino Mass !

Page 46: 何红建 清华大学

RSC, DAD, HJH

Page 47: 何红建 清华大学
Page 48: 何红建 清华大学

VLHC: http://vlhc.org (50-200TeV)

Page 49: 何红建 清华大学

Lessons: (1) A Good Theory ! (2) Vigorous Experiments !! (3) Courage !!!

Page 50: 何红建 清华大学

Origin of Masses, TeV Scale & LHCOrigin of Masses, TeV Scale & LHC

Why TeV Scale:Why TeV Scale: ( ( Strongest BoundStrongest Bound is from is from Unitarity ! Unitarity ! ))

Unitarity of WUnitarity of WLLWWLL → W → WLLWWLL ( < 1.2TeV ) ( < 1.2TeV )

JustifyJustify 1TeV Scale 1TeV Scale forfor LHC + ILC !! LHC + ILC !!

What New PhysicsWhat New Physics: : Higss vs HiggsLess Higss vs HiggsLess + SPV

Light Higgs or Heavy Higgs or HiggsLess;Light Higgs or Heavy Higgs or HiggsLess; 4d 4d DeconstructionDeconstruction vs Extra-dim vs Extra-dim →→Unitarity Unitarity !! New Spin-1 Gauge Bosons Restore Unitarity !!New Spin-1 Gauge Bosons Restore Unitarity !!

How to Observe How to Observe New Gauge BosonsNew Gauge Bosons:: SignalsSignals vs Bkgndsvs Bkgnds

LHC is very Promising to find LHC is very Promising to find WW11 by 2011-12 !!!by 2011-12 !!!                   

Conclusions: