ilc tdr v2: physics, arxiv:1306.6352 heinemeyer @ ilc tdr launch lykken @ ilc tdr launch brock and...

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ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013 H Yamamoto @ LP 2013 H Murayama @ LP2013 Various Google Images 10th LHC Physics Monthly Meeting @ KIAS on 13/Dec/2013 S.Y. Choi (Chonbuk, Korea) LHC ILC Physics : Why & How Introduction (ILC) Standard Physics (Higgs) New Physics (SUSY) How to go ahead

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LHC ☞ ILC Physics : Why & How . S.Y. Choi (Chonbuk, Korea). ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013 H Yamamoto @ LP 2013 H Murayama @ LP2013 Various Google Images …. - PowerPoint PPT Presentation

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Page 1: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

ILC TDR v2: Physics, arXiv:1306.6352Heinemeyer @ ILC TDR Launch

Lykken @ ILC TDR LaunchBrock and Peskin @ Snowmass 2013

Shipsey @ Snowmass 2013H Yamamoto @ LP 2013H Murayama @ LP2013Various Google Images

10th LHC Physics Monthly Meeting @ KIAS on 13/Dec/2013

S.Y. Choi (Chonbuk, Korea)LHC ☞ ILC Physics : Why &

How

Introduction (ILC)Standard Physics (Higgs)

New Physics (SUSY)How to go ahead

Page 2: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Introduction

Page 4: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Neutrino Mass Theory of Flavor

Higgs Boson NaturalnessMatter Asymmetry

Dark MatterDark Energy

Inflation…

What we know is a droplet, while

what we don’t know is an ocean

Mysteries of the Universe (a partial list)[Fermi Today

Nov/15, 2013]

TeV-scale

Page 5: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Scenarios ⇔ Questions

Page 6: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

I attach more value to finding a fact, even about the slightest thing, than to lengthy disputa-tions about the Greatest Ques-

tions that fail to lead to any truth whatever.

Galileo Galilei [Quigg]

Page 7: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Higgs-dependence Day

Page 8: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Perfect?Higgs Lamp Post

MH = 125 GeV JP = 0+

v=246 GeV ↓

m[W, Z, f, H]

[H Murayama]

[Nobel prize website]

Page 9: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

3 Major Frontiers

Omni-directional Exploration

Page 10: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Precision experimentsDiscovery through inducing quantum loops

Neutrino experimentsDiscovery by inducing quantum mixing

Astrophysical experimentsDiscovery by capturing cosmic quanta

Colliding beam experimentsDiscovery by producing on-shell states

Entangled Approaches

Page 11: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Energy Frontier Proposals

[For details, Yamamoto’s talk]

Page 12: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

LHC ☞ ILC

real design[Yokoya’s talk]

Most feasible and realistic

Page 13: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

[Yokoya & ES Kim][Yamamoto & IH Park]

Two-minute Introduction

Clean and Controllable

Page 14: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013
Page 15: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Physics at the ILC : determined by experimental data

A Higgs particleTop quark

Gauge bosons : W and Z…

Clear physics case

“Likely” (additional) physics case

Anomalous (g-2)μDark matter

[SH Jung’s talk]

Clarified more by next LHC experiments

GigaZ

Page 16: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Standard Physics (Higgs)

[For details, see Tanabe’s talk]

Precision

Page 17: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

The new world with a Higgs discovery

Time to analyze!!!

Urgent experimental checks for the SM Higgs boson or not

elementary and single?

Any deviation ⇒ BSM physics!

Page 18: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Outline of a precision Higgs programExperimental and theoretical requirements

Projections of Higgs coupling accuracyMeasurement potential at future colliders

Projection of Higgs property studiesMass, spin-parity, CP mixture, etc

Extended Higgs boson sectorsPhenomenology and prospects for discovery

Higgs Themes

[P Ko’s talk]

Page 19: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Models with new TeV-scale particles give corrections to Higgs couplings of a few %

An experimental program to determine these couplings is achievable

LHC is the facility to study Higgs in the next decadeInteresting precision begins with 300/fb runningSuccess requires considerable theoretical effort

Lepton colliders are required in order to measure sub-% precision in couplings

in a model-independent fashionWith access to invisible and exotic decay modes

Higgs Couplings

Page 20: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Model-independent x-section and coupling measurement

A dream case

Page 21: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

New particles are around 1 TeV

Coupling measure-ments

[For details, see Tanabe’s talk]

Page 22: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Clear and big improvement from ILC measurements?!

[Peskin]

Page 23: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Any deviation from the straight line ⇒ BSM physics

Putting everything together

SM Higgs Mechanism: Mass ∝ Coupling

[ILC TDR 2013]

Page 24: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Precision neutral-current measurements predicted MW/Z

UA1/UA2 discovered W/Z bosonsLEP nailed the SM gauge sector

Precision W/Z measurements predicted MH LHC discovered a Higgs particle

ILC nails the Higgs sector

Precision H measurements predict ?

?????

Repeated History of Collider Experiments?

[H Murayama]

Page 25: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

New Physics(SUSY)

[For details, see Tanabe’s talk]

Complementary

Page 26: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

The questions of fine tuning is still openDark matter (particle) is not included

Neutrino masses are not included(g-2)μ with ~4σ discrepancy

Gravity is not included…

TeV-scale particle candidates

Weakly coupled: SUSY, DM, Long-livedStrongly coupled/composite: RS, KK and Z’, long-lived

…Evolution towards robust search strategies

SM is NOT the ultimate theory

Page 27: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Natural hierarchy, unification, DM, (g-2)μ, more Higgs bosons, etc

SUSY as a Show CaseStill the best BSM scenario?!

Page 28: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Case 1: DM – Is it a particle?

“Particle concept” has been working so far!

[Ellis, 2013]

Page 29: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

DM : Lightest neutralino

DM could be reconstructed to match astrophysical data!?

[ILC TDR 2013]

Page 30: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Case 2: Anomalous (g-2)μ

[Benayoun, David, DelBuono, Jegerlehner, 2012]

More than 4 σ deviation ⇒ real? SM physics?!

Page 31: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

SUSY easily explains the deviation

Experimental data indicatenot too heavy smuons /sneutrinos

not too heavy charginos/neutralinos

Precision SUSY spectroscopy at ILCif kinematically accessible

Page 32: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

[ILC TDR 2013]

(sub)per-cent precision possible at ILC

Precision ILC analyses

Page 33: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Case 3: Light Higgs below 125 GeV

The discovered 125 GeV Higgs might not be the lightest Higgs in the spectrum!

Several light Higgs bosons ⇒ Rich Higgs phenomenology

Constraints

Direct searches for the lightest HiggsDirect searches for other heavier neutral Higgses

Direct searches for the charged HiggsesFlavor constraints (e.g. Bs to muon pairs)

Page 34: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

LHC

ILC

Could be a unique opportunity for the ILC!

Page 35: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Crucial to take into account all decay channels

Huge reduction of excluded parameter space

[Heinemeyer @ LCWS 13]

Page 36: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

[Heine-meyer]

Page 37: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Case 4: LHC finds only a SM-like Higgs and nothing else

ILC + GigaZ

Precise Higgs measurement (ILC)Precision observable measurements (GigaZ)

Precise top measurement (ILC+GigaZ)

Any significant deviations from the SM

predictions could be observed at ILC

Page 38: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

How to go ahead

Page 39: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013
Page 40: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013
Page 41: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

A Meaningful Majority Opinion

Discovery of a Higgs particle together with W/Z, top, DM, (g-2)μ, … comprises a perfect

physics case for the ILC

Staged ApproachesILC as a Higgs and top factory

Start at lower energies to produce ~0.1 million Higgs bosonsGo to higher energies for top physics

Go to higher energies for Higgs + top and Higgs self-couplings

Go to higher energies for TeV scale explorationor

Other options : GigaZ, photon colliders etc

Page 42: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

The Higgs discovery marks the dawn of a new era!

ILC, fueled by a global program on many fronts, canget us to a new paradigm of fundamental physics!!

ILC on the Launch Pad [Lykken]

Page 43: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Back-up Slides

Page 44: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

2013 Nobel Prize in Physics

Page 45: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013
Page 46: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Higgs Self-Coupling

Page 47: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Clear and strong improvement from ILC measurements??

[SFitter 2013]

Page 48: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Higgs Mass and Width

Page 49: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013
Page 50: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013
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Page 57: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Perfect agreement with the Standard Model

Page 58: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013
Page 59: ILC TDR v2: Physics, arXiv:1306.6352 Heinemeyer @ ILC TDR Launch Lykken @ ILC TDR Launch Brock and Peskin @ Snowmass 2013 Shipsey @ Snowmass 2013

Energy 7-14 TeV 0.25 – 1 TeV

Useful energy partly all

Beam proton (com-plex)

electron (point)

Signal high low

noise very high low

analysis specific almost all

events not all all

status real R&D

LHC ⇔ ILC

www.cern.ch www.linearcollider.orgwww.interactions.org