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Hunting for New Particles & Forces

Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

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Page 1: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Hunting for New Particles

&Forces

Page 2: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Example: Two particles produced

• Animations:• QPJava-22.html

u

u

d

u

d

u

Page 3: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Example: Dark Matter Particle produced

• Animations:• QPJava23.html

u

u

d

u

d

u

Page 4: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Physics at the Tevatron

mb -

b -

nb -

pb -

fb -

100 120 140 160 180 200- - - -

Higgs Mass [GeV/c2]

Total Inelastic

bb

WZ

tt-

-

WZ

Tevatron

3 x 1014

2 x 1011

6 x 107

2 x 107

28,00016,000, 12,000

HiggsWH,ZH 4000 ~ 400

400 ~ 40

jets (qq, qg, gg)

Single Top

obse

rved

Page 5: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Tevatron Cross Sections

The Higgs cross section is10-11 orders of magnitudes lower than the total inelastic cross section.

Recent evidence of single top quark production is an important milestone towards the Higgs boson.

Light quarks are ubiquitous.

Plenty of W and Z bosons → calibration.

Total inelastic cross section.

Page 6: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

W

W

top

bottom

Higgs

Tevatron: Improve Higgs Mass Pred. via Quantum Corrections

Mtop (GeV)

MW

(GeV

)

150 175 200

80.5

80.4

80.3

1 GeV = 1 GeV / c2 ~ proton mass

M higgs

= 1

00 G

eV20

0 GeV

300

GeV

500

GeV

1000

GeV

Page 7: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

W

top

bottom

Z

top

topW, Z

Higgs

Tevatron: Higgs Mass Prediction via Quantum Corrections

Clues to the Higgs ?

MH = 92+45-32 GeV;

MH < 186 @ 95% CLMtop (GeV)

Tevatron Run II

MW

(GeV

)

Page 8: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Tevatron: Higgs Mass Prediction via Quantum Corrections

Clues to the Higgs ?

MH = 76+33-24 GeV; 114 < MH < 182 @ 95% CL

Winter 2007Winter 2007

2tW mm 2ln HW mm

Page 9: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Higgs boson production @ Tevatron

• Associated Production• mH < 135 GeV

– (W,Z+H) ¼ 0.15 pb H bb H WW

• Gluon fusion• mH > 135 GeV

– (H) ¼ 0.45 pb

Page 10: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Higgs boson decays• H ff, WW, ZZ

– couples to mass;– heaviest final state

dominates

• mH < 135 GeV– H bb

• mH > 135 GeV– H WW

Tevatron can explore bb and WW(ℓ+ℓ-) decay modes

Page 11: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

SM Higgs: Event SignaturesmH<135 GeV

mH>135 GeV

Page 12: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Status of Direct Search for Higgs boson

• 2010: 8 fb-1

– Exclude115 < mH < 125 GeV and 150 <mH < 180 GeV

Page 13: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

The Next Energy Frontier

The Large Hadron Collider

Page 14: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

SM Higgs boson production• Gluon fusion

• Vector Boson Fusion

• W, Z associated production

• tt, bb associated production

Page 15: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Tevatron: Improve Higgs Mass Pred. via Quantum Corrections

Mtop (GeV)

MW

(GeV

)

LHC: Designed to discover Higgs with Mhiggs = 100 ~ 800 GeV

M (GeV)

130 GeV HiggsL = 100 fb-1

# of

eve

nts

/ 0.

5 G

eV

Tevatron LHC

Page 16: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

MHiggs (GeV)

5 D

isco

very

Lum

inos

ity (

fb-1)

Tevatron: Improve Higgs Mass Pred. via Quantum Corrections

Mtop (GeV)

MW

(GeV

)

LHC: Designed to discover Higgs with Mhiggs = 100 ~ 800 GeV

Tevatron LHC

Page 17: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Mtop (GeV)

MW

(GeV

)

MHiggs (GeV)

5 D

isco

very

Lum

inos

ity (

fb-1)

Tevatron: Improve Higgs Mass Pred. via Quantum CorrectionsLHC: Designed to discover Higgs with Mhiggs = 100 ~ 800 GeV

Tevatron LHC

easy

hard

Will the Tevatron’s prediction agree with what LHC sees?

Page 18: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

tan

MA (GeV)

LHC

Mtop (GeV)

MSSM

MW

(GeV

)

TevatronLHC

Tevatron LHC

Higgs in Minimal Supersymmetric Extension of Standard Model

LHC will be the best place to discover Higgs particles!

Page 19: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Unification of the Forces

Page 20: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Unification

We want to believe that there was just one force after the Big Bang.

As the universe cooled down, the single force split into the four that we know today.

1TeV = 103GeV(1016K)10-11 s

1016GeV(1029 K)10-38 s

1019GeV(1032K)10-41 s

2.3 x 10-13 GeV(2.7K)

12x109 y

EnergyTempTime

Page 21: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Unification of electromagnetic & weak forces

(electroweak theory)

Long term goal since 60’sWe are getting there.

Beautifully demonstratedat HERA ep Collider at DESY

The main missing link is Higgs boson

HERA

Q2 [GeV2]

Electromagnetic ForceWeak Force

f

HERA:H1 +ZEUS

Page 22: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

-1

-1

-1

104 108 1012 1016 1020

Q [GeV]

60

40

20

0

-1

13 orders of magnitude higher energy

The Standard Model fails to unify the strong and electroweak forces.

Page 23: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Adding super-partners

Page 24: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

104 108 1012 1016 1020

Q [GeV]

60

40

20

0

-1

-1

-1

-1

With SUSY

Page 25: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

With SUSYUnifying gravity with the other 3 is accomplished by string theory.

String theory predicts extra hidden dimensions in spacebeyond the three we sense daily.

Other models predict large extra dimensions:large enough to observe up to multi TeV scale.

Page 26: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Extra Dimensions?• Attempts to unify gravity with other forces predicts extra dimensions.• Explains why gravity appears weak.• These extra dimensions could be very small, which is why we don't see

them. – To a tightrope walker, the tightrope is one-dimensional: he can only move

forward or backward

– But to an ant, the rope has an extra dimension: the ant can travel around the rope as well

Page 27: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Large Extra Dimensions of Space

LHC can discover partner towers up to a given energy scale.

qq,gg GN e+e-,+-

Mee, [GeV]

LHC

Mee [GeV]

DZero

Tevatron

GNq

q

e+

e-

Tevatron Sensitivity2.4 TeV @95% CL

Mee [GeV]

Eve

nts

/ 50

GeV

/ 1

00 f

b-1

102

10

1

10-1

10-2

LHC

Page 28: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

New forces of nature new gauge boson

LHC has great discovery potential for multi TeV Z’.

Mee [GeV] M [GeV]

Tevatron LHC 104

103

102

10

1

10-1

Events/2GeV

qq Z’ e+e-

Tevatron sensitivity~1 TeV

CDF Preliminary

Little Higgs Models ? New strong Dynamics ?

Page 29: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

New Particles?

• Solution to the dark matter problem?

Page 30: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

We are hoping in the next ~5 years we will discover Higgs. This will open windows for discovering new laws of nature.

Discovering “laws of nature” is exciting!!

Page 31: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Physics Beyond Borders

Page 32: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u
Page 33: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Why high energy?

E= hc

(courtesy Louis de Broglie)

Visible light 10-6 mElectron microscope 10-10 mRutherford's a-particles 10-14 m1 TeV protons 10-18 m

Smallest length scale probed

Page 34: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u
Page 35: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Particles Tell Stories!

The discovery of a new particle is often the opening chapter revealing unexpected features of our universe.

Particles are messengers telling a profound story

about nature and laws of nature in microscopic world.

The role of physicists is to find the particles and to listen to their stories.

Page 36: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

What is the story they may tell…

Page 37: Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u

Entire new particle spectrum?Super Symmetry

– Attempting to unify gravity with the other fundamental forces leads to a startling prediction:

• every fundamental matter particle should have a massive "shadow" force carrier particle, and every force carrier should have a massive "shadow" matter particle. ….

http://www.particleadventure.org