physics at the high energy frontier j. hewett panic 2005

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Physics at the High Energy Frontier J. Hewett PANIC 2005

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Page 1: Physics at the High Energy Frontier J. Hewett PANIC 2005

Physics at the High Energy Frontier

J. Hewett PANIC 2005

Page 2: Physics at the High Energy Frontier J. Hewett PANIC 2005

What is the world made of?What holds the world together?

Where did we come from?

Primitive Thinker

Courtesy: Y.K. Kim

Page 3: Physics at the High Energy Frontier J. Hewett PANIC 2005

Evolved Thinker

From “Quantum Universe”

Courtesy: Y.K. Kim

1. Are there undiscovered principles of

nature: New symmetries, new physical laws?

2. How can we solve the mystery of dark

energy?3. Are there extra dimensions of

space?4. Do all the forces become one?5. Why are there so many kinds of

particles?6. What is dark matter? How can we make it in the

laboratory?7. What are neutrinos telling us?8. How did the universe come to be?9. What happened to the antimatter?

Page 4: Physics at the High Energy Frontier J. Hewett PANIC 2005

LHC:

ILC:

Collider Tools which Answer these Questions:

proton proton

e- e+

•Broad energy reach•Large event rate

•Knowledge of initial quantum state•Well-defined initial energy and angular momentum (polarization)•Clean environment•Can vary CoM

Page 5: Physics at the High Energy Frontier J. Hewett PANIC 2005

The LHC is Becoming a Reality!

The excitement is building - we are counting down the days….

Page 6: Physics at the High Energy Frontier J. Hewett PANIC 2005

Major Discoveries are Expected!

- A. De Roeck, Snowmass 2005

Page 7: Physics at the High Energy Frontier J. Hewett PANIC 2005
Page 8: Physics at the High Energy Frontier J. Hewett PANIC 2005

Much Progress on the ILC in the Last Year:•Superconducting rf Technology chosen •Global Design Effort Launched!

Barry Barrish is Director of the GDE

+ 3 Regional Directors+ 45 Team Members and counting…

Baseline Configuration being Defined now…

Page 9: Physics at the High Energy Frontier J. Hewett PANIC 2005

Barrish, Snowmass 05

Page 10: Physics at the High Energy Frontier J. Hewett PANIC 2005

Barrish, Snowmass 05

Page 11: Physics at the High Energy Frontier J. Hewett PANIC 2005

Particles Tell Stories: Discovery of a new particle is the opening chapter of a story. These particles are merely the messengers which reveal a profound story about the nature of matter, energy, space, and time.Learning the full story involves:1) Discovery of a new particle2) Discovery of the theory behind the new

particleIt is up to us to find the new particles and to listen to their stories

Page 12: Physics at the High Energy Frontier J. Hewett PANIC 2005

Particles Tell Stories: Discovery of a new particle is the opening chapter of a story. These particles are merely the messengers which reveal a profound story about the nature of matter, energy, space, and time.Learning the full story involves:1) Discovery of a new particle2) Discovery of the theory behind the new

particle

Measurements at the ILC, together with results from the LHC, will identify the full nature of the physics at the TeV scale and reveal its full story

It is up to us to find the new particles and to listen to their stories

Page 13: Physics at the High Energy Frontier J. Hewett PANIC 2005

HEPAP LHC/ILC Subpanel Report(s):

•43 page semi-technical version, submitted to EPP2010 panel in late Julyhttp://www.science.doe.gov/hep/LHC-ILC-Subpanel-EPP2010.pdf

•35 page non-technical version, in press.

The report emphasizes:• the synergy between the LHC and ILC• differences in how measurements are made at ILC and LHC•unique physics to ILC

Page 14: Physics at the High Energy Frontier J. Hewett PANIC 2005

The Authors:

Page 15: Physics at the High Energy Frontier J. Hewett PANIC 2005

The report centers on 3 physics themes:

1. Mysteries of the Terascale: Solving the mysteries of matter at the Terascale

2. Light on Dark Matter: Determining what Dark Matter particles can be produced in the laboratory and discovering their identity

3. Einstein’s Telescope: Connecting the laws of the large to the laws of the small

Now for some highlights of physics unique to the ILC

Page 16: Physics at the High Energy Frontier J. Hewett PANIC 2005

Higgs at the Terascale• An important Higgs production process

is e+e- Z + Higgs

• There are many possible final states, depending on how the Z and Higgs decay In e+e- Z + Anything

•‘Anything’ corresponds to a system recoiling against the Z •The mass of this system is determined solely by kinematics and conservation of energy•because we see everything else, we know what is escaping

Recoil Technique:

Peak in Recoil Mass corresponds to 120 GeV Higgs!

Page 17: Physics at the High Energy Frontier J. Hewett PANIC 2005

ILC Simulation for e+e- Z + Higgswith Z 2 b-quarks and Higgs invisible

N. Graf

Page 18: Physics at the High Energy Frontier J. Hewett PANIC 2005

Provides accurate, direct, and Model Independentmeasurements of the Higgs couplings

Recoil technique gives precise determination of Higgs properties Independent of its decay mode

•The strength of the Higgs couplings to fermions and bosons is given by the mass of the particle

•Within the Standard Model this is a direct proportionality

This is a crucial test of whether a particle’s mass is generated by the Higgs boson!

Higgs

f

f-

~ mf

Page 19: Physics at the High Energy Frontier J. Hewett PANIC 2005

Size of measurement errors

ILC will have unique ability to make model independent tests of Higgs couplings at the percent level of accuracy.

mh = 120 GeV

Page 20: Physics at the High Energy Frontier J. Hewett PANIC 2005

Possible deviations in models with Extra Dimensions This is the right

sensitivity to discover extra dimensions, new sources of CP violation, or other novel phenomena

Mass (GeV)

mh = 120 GeV

Cou

plin

g s

tren

gth

to H

igg

s

boson

Higgs is Different! First fundamental scalar to be discovered: could be related to many things, even dark energy

Page 21: Physics at the High Energy Frontier J. Hewett PANIC 2005

ILC Studies superpartners individually via e+e- SSDetermines•Quantum numbers (spin!)•Supersymmetric relation of couplings

= e

~~ = 2e

-

Proof that it IS Supersymmetry!

Supersymmetry at the Terascale

M1 (GeV)

Rati

o o

f C

ou

plin

g S

treg

ths

Selectron pair production

2% accuracy in determination of Supersymmetric coupling strength

Page 22: Physics at the High Energy Frontier J. Hewett PANIC 2005

Precise Mass Measurements of SuperpartnersExample: e e +

Fixed center of mass energy gives flat energy distribution in the laboratory for final state e- Endpoints can be used to determine superpartner masses to part-per-mil accuracy

~ ~

e

A realistic simulation:

Determines Superpartner masses of the electron and photon to 0.05%!

Page 23: Physics at the High Energy Frontier J. Hewett PANIC 2005

A complicated Table with lots of details that illustrates how ILC results improve upon Superpartner mass measurements at the LHC

Shows accuracy of mass determinations at LHC and ILC alone and combined

Page 24: Physics at the High Energy Frontier J. Hewett PANIC 2005

Accurate superpartner mass determinations necessary for unification tests

Evolution of superpartner masses to high scale:

Force unification Matter Unification

Einstein’s Telescope to Unification

Page 25: Physics at the High Energy Frontier J. Hewett PANIC 2005

•Kaluza-Klein modes in a detector

104

106

108

104

106

108

Number of Events in e+e- +-

For a conventional braneworld model with a single curved extra dimension of size ~ 10-17

cm

For this same model embedded in a string theory

Standard Model Z-boson

1st KK mode 2nd KK

mode3rd KK mode

Extra Dimensions at the Terascale

Page 26: Physics at the High Energy Frontier J. Hewett PANIC 2005

Detailed measurements of the properties of KK modes can determine:

•That we really have discovered additional spatial dimensions

•Size of the extra dimensions

•Number of extra dimensions

•Shape of the extra dimensions

•Which particles feel the extra dimensions

•If the branes in the Braneworld have fixed tension

•Underlying geometry of the extra dimensional space

Page 27: Physics at the High Energy Frontier J. Hewett PANIC 2005

Example: Production of Graviton Kaluza-Klein modes in flat extra dimensions, probes gravity at distances of ~ 10-18 cm

Production rate for e+e- + Graviton

104

105

106

with

7Extra Dimensions6

5

4

3

2

Size of Measurement error

Measurement possible due to well-defined initial state & energy plus clean environment

Page 28: Physics at the High Energy Frontier J. Hewett PANIC 2005

Where particles live in extra dimensions

Polarized Bhabha Scattering

Determines location of left- and right-handed electron in extra dimension of size 4 TeV-1

Locati

on

of

eL in

an

extr

a d

imen

sio

n

Location of eR in an extra dimension

Page 29: Physics at the High Energy Frontier J. Hewett PANIC 2005

Telescope to Very High Energy Scales

‘X’

Many tools to detect existence of heavy object ‘X’:•Deviations in production rates•Deviations in production properties such as distribution of angle from beam-line•Deviations in distributions of angular momentum

For all types of final state fermions!

ILC can probe presence of Heavy Objects with Mass > Center of Mass Energy in e+e ff

Indirect search for New Physics

-

Page 30: Physics at the High Energy Frontier J. Hewett PANIC 2005

Various Unification Models

For ILC Sensitivity:Solid = 5 = standard discovery criteria

Dashed = 2

95% (=2) direct discovery at LHC

Example: New Heavy Z-like Boson from Unification Theories

Collider Sensitivity

Mass of Z-like Boson (TeV)ILC can probe masses many times the machine energy!

Page 31: Physics at the High Energy Frontier J. Hewett PANIC 2005

95% contours for Z’ couplings to leptons at ILC

LHC determines massILC determines interactions

Nu

mb

er

of

Even

ts in

pp

+-

Mass of muon pair (TeV) Axial Coupling

Vecto

r C

ou

plin

gKaluza-Klein Z’

SO(10): origin of massE6:

unified Higgs

Drell-Yan distribution at LHC

Page 32: Physics at the High Energy Frontier J. Hewett PANIC 2005

Light on Dark Matter

•Dark Matter comprises 23% of the universe

•No reason to think Dark Matter should be simpler than the visible universe likely to have many different components

•Dream: Identify one or components and study it in the laboratory

Page 33: Physics at the High Energy Frontier J. Hewett PANIC 2005

•A component of Dark Matter could be the Lightest Neutralino of Supersymmetry - stable and neutral with mass ~ 0.1 – 1 TeV•In this case, electroweak strength annihilation gives relic density of

m2

ΩCDM h2 ~ (1 TeV)2

One Possibility: Dark Matter in Supersymmetry

Page 34: Physics at the High Energy Frontier J. Hewett PANIC 2005

Comparative precision of ILC measurements (within SUSY)

ILC and Astro measurements

ILC and direct detection

Page 35: Physics at the High Energy Frontier J. Hewett PANIC 2005
Page 36: Physics at the High Energy Frontier J. Hewett PANIC 2005

The more discoveries that are made at the LHC, the greater the discovery potential at the ILC

Page 37: Physics at the High Energy Frontier J. Hewett PANIC 2005

The more discoveries that are made at the LHC, the greater the discovery potential at the ILC

When the LHC makes its discoveries, let’s be ready to start construction on the ILC!