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2nd ANNUAL MEETING of the PRAIRIE SECTION of the AMERICAN PHYSICAL SOCIETY held in conjunction with the Chicago Section of the American Association of Physics Teachers (CSAAPT) THE COMING REVOLUTIONS IN PARTICLE PHYSICS 1

THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

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Page 1: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

2nd ANNUAL MEETING of the PRAIRIE SECTION of the AMERICAN PHYSICAL SOCIETYheld in conjunction with the Chicago Section of the American Association of Physics Teachers (CSAAPT)

Thursday, November 18, 7:00 p.m.Wishnick Hall AuditoriumIIT Main Campus, Chicago, IL

Students, faculty, alumni, IIT Community are welcome to this free public lecture.

The Large Hadron Collider provides the greatest leap in capability of any instrument in the history of particle physics. We do not know what it will find, but the discoveries we make and the new puzzles we encounter are certain to change the face of particle physics and to echo through neighboring sciences.

Join us as we welcome Chris Quigg, the highly respected physicist at the forefront of today’s revolutions in particle physics. His work ranges over many topics, from electroweak symmetry breaking and supercollider physics to heavy quarks and the strong interaction among them to ultrahigh-energy neutrino interactions.

THE COMING REVOLUTIONS IN PARTICLE PHYSICS

RSVP: Professor Christopher White | [email protected]

Theoretical Physics Department, Fermilab2011 J. J. Sakurai Prize for Theoretical Particle Physics Recipient

CHRIS QUIGG1

Page 2: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

The Coming Revolutions in Particle Physics

Chris Quigg

2

Page 3: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Atoms became real in the 20th century

3

Page 4: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

To explain a complicated visible by a simple invisible

Eric

Wee

ks, E

mor

y U

.

Jean Perrin

4

Page 5: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

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Page 6: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

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Page 7: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

All things are made of atoms–little particles that move around in perpetual motion, attracting each other when they are

a little distance apart, but repelling upon being squeezed

into one another.

—Richard Feynman, Six Easy Pieces

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Page 8: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Quantum Mechanics

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Page 9: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Great Lesson of XXth Century Science

The human scale of space & time is not privileged for understanding Nature . . .

and may even be disadvantaged

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Page 10: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

The world’s most powerful microscopes

Tevatron collider at Fermilabprotons on antiprotons at 1+1 TeV

speed of light: c ≈ 109 km/h (30 cm/nanosecond)speed of proton: c – 495 km/h

Protons pass my window 45,000 times / second>10 million collisions per second

10

Page 11: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

D0

CDFCQ

www.fnal.gov

11

Page 12: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

CDF Experiment

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Page 13: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

CDF two-jet event (70% of energy ⊥ beam direction)

quark + antiquark → jet + jet

The World’s Most Powerful Microscopesnanonanophysics

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Page 14: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Walk of Ideas, Altes Museum Berlin (2006)

Lien

hard

Sch

ulz

(Wik

iped

ia)0

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D0 top quark + antiquark

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Page 15: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Accelerators as time machines …

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Page 16: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Pointlike (r ≤ 10−18 m) quarks and leptons

Our Picture of Matter (the revolution just past)

uRdR

cRsR

tRbR

eR

R

R

uLdL

cLsL

tLbL

eLL

L12

3

1

2

3

d u

u

Gravitation, electromagnetism, radioactivity, strong interaction

16

Page 17: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

New Law of Nature #1

Quantum chromodynamics (QCD): color symmetry among quarksred· green· blue gluons

d u

u

D. Leinweber

uRdR

cRsR

tRbR

uLdL

cLsL

tLbL

17

Page 18: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

M78· SDSS

Lattice QCD: quark confinement origin of nucleon masshas explained nearly all visible mass in the Universe

18

Page 19: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

New Law of Nature #2

uLdL

cLsL

tLbL

eLL

Le

Electroweak theory:family symmetryu ↔ d ; ν ↔ e ; …

weak bosons (W+, W–, Z0) + photon

19

Page 20: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Weak interactions, electromagnetism seem so different …

Weak Electromagnetic

range: 1% proton size infinite range

W: 90 × proton mass massless photon

How can they share a common origin (symmetry)?

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Page 21: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Symmetry of laws �⇒ symmetry of outcomes

Stud

ies

amon

g th

e Sn

ow C

ryst

als

... by

Wils

on B

entle

y, vi

a N

OA

A P

hoto

Lib

rary

21

Page 22: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Meissner Effecthidden EM symmetry

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Page 23: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

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Page 24: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Superconductivity suggestsa field that permeates all of spacecould hide electroweak symmetry

Peter Higgs+ R. Brout, F. Englert, G. Guralnik, R. Hagen, T. Kibble

24

Page 25: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Higgs boson: massive particle with spin zerohides electroweak symmetry

gives mass to W and Zgives mass to electron, quarks, etc.

Not yet observed!

Theory does not predict Higgs-boson mass

“Standard” Electroweak Theory

25

Page 26: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Gedankenexperiment

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Page 27: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

100 150 200 250 300

!! 2

0

2

4

6

8

10

12

LEP

excl

usio

n at

95%

CL

Teva

tron

exc

lusi

on a

t 95%

CL

Theory uncertainty

Fit including theory errors

Fit excluding theory errors

MH (GeV)

3!

2!

1!

G fitter SM

March 2009

Where the (standard) Higgs boson might be

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Page 28: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Large Hadron Collider· CERN

proton-proton collisions at 3.5 → 7 TeV/beam

LHCb

ATLASALICE

CMS

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Page 29: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

CMS

29

Page 30: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

CMS

30

30

Page 31: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

CMS

31

Page 32: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

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ATLAS

32

Page 33: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Das LHC Projekt S.Bethke Max-Planck-Institut für Physik 3320

ATLAS

33

Page 34: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

ATLAS

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Page 35: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Fabiola Gianotti (ATLAS) : If we do not find the Higgs boson,that means that the theory is just wrong!

35

Page 36: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

• New kind of force? (Higgs boson)

• New force from a new symmetry?

• Residual force from strong dynamics?

• Echo of extra spacetime dimensions?

Which path has nature taken?

What hides the electroweak symmetry?

36

Page 37: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Why will it matter?

Understanding the everyday …

Why atoms? Why chemistry? Why stable structures?

37

Page 38: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Without a Higgs mechanism …

Electron and quarks would have no massQCD would confine quarks into protons, etc. Proton mass little changedSurprise: QCD would hide EW symmetry, give tiny masses to W, ZMassless electron: atoms lose integrity No atoms means no chemistry, no stable composite structures like liquids, solids, …

… character of the physical worldwould be profoundly changed

38

Page 39: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Much more to learn …

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Page 40: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Revolution: the meaning of identity

• What makes a top quark a top quark and an electron an electron?

• What sets masses of quarks & leptons?

40

Page 41: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

!"#$

!"#%

!"#&

!"#'

!"#(

!"#!

!""

)*++,-.*/01*2.

13*45.6 2.789:+

;7 <;*4/+

69=: <;*4/+

.

;6

1

+

8

>

!

"

Higgs boson knows something we don’t know!41

Page 42: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

KATRIN aims at 0.2 eV

42

Page 43: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Strings?

1018

Planck scale

Quantum gravity?

[A PUZZLE RAISED BY THE HIGGS]

Unexplained gap

Limit of LHC

Strong-electro

weak

uni!cation sc

ale?

Electroweak scale

Electron

Neutrino masses

Muon

Top

Bottom

Tau

Charm

Proton

Neutron

10–6

10–3

100

103

106

109

1012

1015

10–9

HiggsUp Down

Strange ZW

H

Energy Scale (GeV)

An electroweak puzzle:Does MH < 1 TeV make sense?The peril of quantum corrections

Scientific American

43

Page 44: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

How to separate electroweak, higher scales?

Extend electroweak theory on the 1-TeV scale …

composite Higgs boson

technicolor / topcolor

supersymmetry

Ask instead why gravity is so weak

44

Page 45: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

MPlanckM*1/R(1 mm)�–1

1 TeV

Stre

ngth

of F

orce

s3-2-1

LED

Conventional Gravity

Suppose at scale R … gravity propagates in 4+n dimensions

1/r 2

1/r 2+n

MPlanck would be a mirage!45

Page 46: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Range !G (meters)

Lamoreaux

Irvine

Eöt-Wash

Boulder

10–6 10–5 10–4 10–3 10–2

108

104

100

10–4

Rel

ativ

e S

tren

gth "

G

Stanford

Gravity follows Newtonian force law down to ≲ 1 mm

1 0.110E (meV)A

nom

alou

s C

oupl

ing

46

Page 47: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Another “minor” problem

• Higgs field fills all of space with energy density 1028 g/liter

• But empty space weighs next to nothing: < 10-26 g/liter

• New evidence that vacuum energy is present (accelerating universe)

47

Page 48: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

New physics in the LHC range?More

If dark matter interacts weakly …

… its likely mass is 0.1 to 1 TeV

COSMOS

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Page 49: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Dark matter relics of the big bang?

49

Page 50: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Revolution:Unity of Quarks & Leptons

•What do quarks and leptons have in common?

•Why are atoms neutral?

50

Page 51: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Conjectured Law of Nature?

eLL

Le

uLdL

cLsL

tLbL

A symmetry among quarks and leptons …… would have to be a hidden symmetry

eLL

Le

uLdL

cLsL

tLbL

Extended quark–lepton families: proton decay!

51

Page 52: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

SU(3)c

SU(2)L

U(1)Y

log10

�E

1 GeV

1/α

60

40

20

0 5 10 15

Unification of Forces?

52

Page 53: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Connections …

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Page 54: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

ALICE Experiment: Pb-Pb Collisions at 287 TeV

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Page 55: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

?55

Page 56: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

“It was as if, suddenly, we had broken into a walled orchard, where protected trees had flourished and all kinds of exotic fruits had ripened in great profusion.”

— Cecil Powell1950 Nobel Prize

56

Page 57: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

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Page 58: THE COMING REVOLUTIONS IN PARTICLE PHYSICSlutece.fnal.gov/Talks/PrairieRevolutions.pdfare welcome to this free public lecture. The Large Hadron Collider provides the greatest leap

Thanks to …

Eric Weeks for the film of Brownian motion www.physics.emory.edu/~weeks

J. D. Jackson for the photo of Peter Higgs

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