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What is the Universe Made Of? The case for Dark Matter and Dark - - PowerPoint PPT Presentation

What is the Universe Made Of? The case for Dark Matter and Dark Energy, and for what they might be Cliff Burgess What is the Universe Made Of? From best fits to the Concordance Cosmology Courtesy: Ned Wrights Cosmology Page Taipei


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SLIDE 1

What is the Universe Made Of?

The case for Dark Matter and Dark Energy, and for what they might be Cliff Burgess

slide-2
SLIDE 2

What is the Universe Made Of?

From best fits to the ‘Concordance Cosmology’

Courtesy: Ned Wright’s Cosmology Page

Taipei June 2014

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SLIDE 3

What is the Universe Made Of?

From best fits to the ‘Concordance Cosmology’

Courtesy: Ned Wright’s Cosmology Page

Taipei June 2014

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SLIDE 4

1905 – A Big Year for Einstein

  • Photo-electric Effect
  • “On a Heuristic Point of View concerning the Production

and Transformation of Light.” rcd Mar 18, pub Jun 9

  • Brownian Motion
  • “On the Movement of Small Particles Suspended in

Stationary Liquids Required by the Molecular-Kinetic Theory of Heat.” rcd May 11, pub Jul 18

  • Special Relativity
  • “On the Electrodynamics of Moving Bodies.” rcd Jun 30,

pub 26 Sep

  • Size of Molecules
  • “A New Determination of Molecular Dimensions.” rcd

Aug 19, pub Feb 8

  • Mass-Energy Equivalence
  • “Does the Inertia of a Body Depend upon Its Energy

Content?” rcd Sep 27, pub Nov 21

Albert Einstein

Taipei June 2014

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SLIDE 5

1905 – A Big Year for Einstein

  • Photo-electric Effect
  • “On a Heuristic Point of View concerning the Production

and Transformation of Light.” rcd Mar 18, pub Jun 9

  • Brownian Motion
  • “On the Movement of Small Particles Suspended in

Stationary Liquids Required by the Molecular-Kinetic Theory of Heat.” rcd May 11, pub Jul 18

  • Special Relativity
  • “On the Electrodynamics of Moving Bodies.” rcd Jun 30,

pub 26 Sep

  • Size of Molecules*
  • “A New Determination of Molecular Dimensions.” rcd

Aug 19, pub Feb 8

  • Mass-Energy Equivalence
  • “Does the Inertia of a Body Depend upon Its Energy

Content?” rcd Sep 27, pub Nov 21

* PhD Thesis and most cited Albert Einstein

Taipei June 2014

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SLIDE 6

Outline

  • Dark Cosmology
  • The Hot Big Bang
  • Dark Matter
  • Evidence for Dark Matter
  • Dark stuff or modified gravity?
  • Dark Energy
  • Why doesn’t the vacuum gravitate?
  • Dark Energy as vacuum energy

Taipei June 2014

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SLIDE 7

Outline

  • Dark Cosmology
  • The Hot Big Bang
  • Dark Matter
  • Evidence for Dark Matter
  • Dark stuff or modified gravity?
  • Dark Energy
  • Why doesn’t the vacuum gravitate?
  • Dark Energy as vacuum energy

Taipei June 2014

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SLIDE 8

Outline

  • Dark Cosmology
  • The Hot Big Bang
  • Dark Matter
  • Evidence for Dark Matter
  • Dark stuff or modified gravity?
  • Dark Energy
  • Why doesn’t the vacuum gravitate?
  • Dark Energy as vacuum energy

Taipei June 2014

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SLIDE 9

Part I

Taipei June 2014

“It is a capital mistake to theorize before one has data. Insensibly one begins to twist facts to suit theories, instead of theories to suit facts.” Sherlock Holmes in A Scandal in Bohemia

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SLIDE 10

Taipei June 2014

The Hot Big Bang

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SLIDE 11

Gravity, Matter & Geometry

  • According to Einstein gravity is really the response of

space and time to the presence of matter.

  • The presence of energy curves space and time.
  • The curvature of space changes how objects move.
  • Knowing how matter is distributed over large scales

tells us the shape and evolution of the Universe.

Taipei June 2014

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SLIDE 12

Courtesy: Sloan Digital Sky Survey WMAP

Matter Distribution

Taipei June 2014

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SLIDE 13

Evidence for an Expanding Universe

  • The sky is dark
  • The Hubble Law
  • The homogeneity and

isotropy of the universe

  • The slower decay of

more distant supernovae

Courtesy: Ned Wright’s Cosmology Page

d H v 

Taipei June 2014

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SLIDE 14

Hot Big Bang

  • Assume Universe once a hot

soup of elementary particles

  • Seek relics of earlier hotter

epochs

  • Use: at high temperatures

particles get broken to their

  • constituents. As universe

cools, bound states form

Taipei June 2014

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SLIDE 15

Hot Big Bang

  • Atoms form below 1000

degrees

  • electrons and nuclei combine

into neutral atoms.

  • Nuclei form below 1010

degrees.

  • Protons and neutrons

combine into nuclei.

Taipei June 2014

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SLIDE 16

Evidence for a Hot Big Bang

  • Primordial element

abundances

  • The cosmic

microwave background

  • TCMB vs distance

Courtesy: Ned Wright’s Cosmology Page

Burles, Nolette & Turner, 1999

Taipei June 2014

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SLIDE 17

Evidence for a Hot Big Bang

  • Primordial element

abundances

  • The cosmic

microwave background

  • TCMB vs distance

Courtesy: Ned Wright’s Cosmology Page

Burles, Nolette & Turner, 1999

Total Mass Density of Atoms

Taipei June 2014

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SLIDE 18

Evidence for a Hot Big Bang

  • Primordial element

abundances

  • The cosmic

microwave background

  • TCMB vs distance

Courtesy: Ned Wright’s Cosmology Page

Burles, Nolette & Turner, 1999

Total Mass Density of Atoms

Taipei June 2014

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SLIDE 19

Evidence for a Hot Big Bang

  • Primordial element

abundances

  • The cosmic

microwave background

  • TCMB vs distance

Courtesy: Ned Wright’s Cosmology Page

Burles, Nolette & Turner, 1999

Total Mass Density of Atoms

Taipei June 2014

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SLIDE 20

Evidence for a Hot Big Bang

  • Primordial element

abundances

  • The cosmic

microwave background

  • TCMB vs distance

Courtesy: Ned Wright’s Cosmology Page

Burles, Nolette & Turner, 1999

Total Mass Density of Atoms

Taipei June 2014

slide-21
SLIDE 21

Evidence for a Hot Big Bang

  • Primordial element

abundances

  • The cosmic

microwave background

  • TCMB vs distance

Courtesy: Ned Wright’s Cosmology Page

Burles, Nolette & Turner, 1999

Total Mass Density of Atoms

Taipei June 2014

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SLIDE 22

Evidence for a Hot Big Bang

  • Primordial element

abundances

  • The cosmic

microwave background

  • TCMB vs distance

Taipei June 2014

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SLIDE 23

Evidence for a Hot Big Bang

  • Primordial element

abundances

  • The cosmic

microwave background

  • TCMB vs distance

WMAP collaboration

CMB Temperature vs Direction

Taipei June 2014

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SLIDE 24

Evidence for a Hot Big Bang

Planck collaboration

CMB Temperature vs Direction

Taipei June 2014

  • Primordial element

abundances

  • The cosmic

microwave background

  • TCMB vs distance
slide-25
SLIDE 25

DARK MATTER

Part II

Taipei June 2014

“Circumstantial evidence is a very tricky thing,” answered Holmes thoughtfully. “It may seem to point very straight to one thing, but if you shift your own point of view a little, you may find it pointing in an equally uncompromising manner to something entirely different.” Sherlock Holmes in The Boscombe Valley Mystery

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SLIDE 26

DARK MATTER

Taipei June 2014

The evidence for it Dark stuff or modified gravity?

“Circumstantial evidence is a very tricky thing,” answered Holmes thoughtfully. “It may seem to point very straight to one thing, but if you shift your own point of view a little, you may find it pointing in an equally uncompromising manner to something entirely different.” Sherlock Holmes in The Boscombe Valley Mystery

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SLIDE 27

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

Taipei June 2014

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SLIDE 28

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

Taipei June 2014

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SLIDE 29

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

Courtesy: Ned Wright’s Cosmology Page

Taipei June 2014

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SLIDE 30

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

The Bullet Cluster: Separating Dark

and Visible Matter

Taipei June 2014

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SLIDE 31

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

The Bullet Cluster: Separating Dark

and Visible Matter

Colliding galaxy clusters

Taipei June 2014

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SLIDE 32

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

The Bullet Cluster: Separating Dark

and Visible Matter

Hot intra-cluster gas

Taipei June 2014

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SLIDE 33

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

The Bullet Cluster: Separating Dark

and Visible Matter

Mass measured by lensing

Taipei June 2014

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SLIDE 34

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

The Bullet Cluster: Separating Dark

and Visible Matter

Taipei June 2014

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SLIDE 35

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

Time available for structure formation

Taipei June 2014

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SLIDE 36

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

Time available for structure formation

Taipei June 2014

log r log a

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SLIDE 37

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

Time available for structure formation

Taipei June 2014

log r log a

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SLIDE 38

Evidence for Dark Matter

  • Mass in galaxies
  • Mass in clusters of

galaxies

  • Temperature

fluctuations in the CMB

  • Start of galaxy

formation

Time available for structure formation

Taipei June 2014

log r log a

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SLIDE 39

What is the Dark Matter?

  • Ordinary atoms?
  • Modifications to

the Law of Gravity?

  • New kind of

particles?

Taipei June 2014

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SLIDE 40

What is the Dark Matter?

  • Ordinary atoms?
  • Modifications to

the Law of Gravity?

  • New kind of

particles?

Burles, Nolette & Turner, 1999

Courtesy: Ned Wright’s Cosmology Page

Taipei June 2014

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SLIDE 41

What is the Dark Matter?

  • Ordinary atoms?
  • Modifications to

the Law of Gravity?

  • New kind of

particles?

The devil is in the details: No proposals yet succeed for galaxies and clusters and the CMB. Very difficult to modify gravity at long distances without having problems with fundamental principles.

Taipei June 2014

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SLIDE 42

What is the Dark Matter?

  • Ordinary atoms?
  • Modifications to

the Law of Gravity?

  • New kind of

particles?

Weakly Interacting Particles arise in most theories of microscopic physics. Their residual cosmic abundance is naturally the right size to agree with the

  • bserved amount of

Dark Matter.

Taipei June 2014

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SLIDE 43

DARK ENERGY

Part III

Taipei June 2014

“How often have I said to you that when you have eliminated the impossible, whatever remains, however improbable, must be the truth?” Sherlock Holmes in The Sign of the Four

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SLIDE 44

DARK ENERGY

Taipei June 2014

Evidence for Dark Energy The Cosmological Constant Problem

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SLIDE 45

Evidence for Dark Energy

  • Brightness of

very distant supernovae

  • Flatness of the

universe as a whole

Taipei June 2014

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SLIDE 46

Evidence for Dark Energy

  • Brightness of

very distant supernovae

  • Flatness of the

universe as a whole

Very distant objects should not precisely follow Hubble’s Law because gravitational attraction should decelerate the universal expansion. This can be tested by looking for deviations from Hubble’s Law for very distant supernovae.

Taipei June 2014

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SLIDE 47

Evidence for Dark Energy

  • Brightness of

very distant supernovae

  • Flatness of the

universe as a whole

Taipei June 2014

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SLIDE 48

Evidence for Dark Energy

  • Brightness of

very distant supernovae

  • Flatness of the

universe as a whole

The universal expansion should be decelerating due to gravitational attraction Expect this:

Taipei June 2014

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SLIDE 49

Evidence for Dark Energy

  • Brightness of

very distant supernovae

  • Flatness of the

universe as a whole

Courtesy: Ned Wright’s Cosmology Page

Tonrey et.al., 2003

Taipei June 2014

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SLIDE 50

Evidence for Dark Energy

  • Brightness of

very distant supernovae

  • Flatness of

the universe as a whole

Courtesy: Ned Wright’s Cosmology Page

Tonrey et.al., 2003

Amount of Dark Matter

Taipei June 2014

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SLIDE 51

Evidence for Dark Energy

WMAP collaboration Small temperature variations, at

the level of one part in 100,000, are visible in the CMB

  • Brightness of

very distant supernovae

  • Flatness of the

universe as a whole

Taipei June 2014

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SLIDE 52

Evidence for Dark Energy

WMAP collaboration

These are due to sound waves in the primordial gas which emitted this light.

  • Brightness of

very distant supernovae

  • Flatness of the

universe as a whole

Taipei June 2014

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SLIDE 53

Evidence for Dark Energy

  • Brightness of

very distant supernovae

  • Flatness of the

universe as a whole

The CMB allows the inference of the properties of the later universe through which these photons pass.

Taipei June 2014

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SLIDE 54

Evidence for Dark Energy

  • Brightness of

very distant supernovae

  • Flatness of the

universe as a whole

Courtesy: Ned Wright’s Cosmology Page

Measurements of CMB and Dark Matter

and universal expansion and acceleration are consistent

Amount of Dark Matter

Taipei June 2014

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SLIDE 55

Concordance Cosmology

Can also count ordinary atoms even if they cannot be seen! Nucleosynthesis Properties of the CMB

Courtesy: Ned Wright’s Cosmology Page

Taipei June 2014

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SLIDE 56

The cosmological term

  • Einstein’s equations as initially written preclude the existence
  • f a static Universe

Taipei June 2014

𝐻𝜈𝜉 + 𝜇 𝑕𝜈𝜉 = 8𝜌𝐻 𝑈

𝜈𝜉

𝐻𝜈𝜉 = 8𝜌𝐻 𝑈

𝜈𝜉

  • This conclusion can be avoided if they are modified to include

a ‘cosmological term’ which acts as a repulsive counterforce to gravity’s attraction

  • The requirement for the cosmological term was removed once

the Universe was found to be expanding.

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SLIDE 57

Cosmological term as Dark Energy

  • The cosmological term provides an excellent description of the

Dark Energy, since its repulsive nature can drive the observed cosmological acceleration

Taipei June 2014

  • Interpreted as a stress-energy the cosmological term looks like

constant positive energy density and negative pressure

8𝜌𝐻 𝑈

𝜈𝜉 = −𝜇 𝑕𝜈𝜉

−𝑞 = 𝜍 = 𝜇 8𝜌𝐻

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SLIDE 58

Einstein’s error

  • Was Einstein’s greatest error introducing the cosmological

term, or discarding it before Dark Energy was discovered?

Taipei June 2014

𝐻𝜈𝜉 = 8𝜌𝐻 𝑈

𝜈𝜉 − 𝜇 𝑕𝜈𝜉 = 8𝜌𝐻 (𝑈 𝜈𝜉 + 𝑢𝜈𝜉)

  • Modern point of view: Neither! His error was to believe he

gets to choose...

  • The cosmological term is precisely what a vacuum energy, 𝑢𝜈𝜉,

would look like, and we should be able to compute its properties if we understand the vacuum.

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SLIDE 59

Vacuum Energy as Dark Energy

  • The success of special

relativity requires the vacuum energy density to be constant and its pressure to be negative, as required to be Dark Energy.

  • Negative pressure keeps the

vacuum energy density constant as the universe expands.

log r log a

     r p

Taipei June 2014

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SLIDE 60

The Cosmological Constant Problem

  • The vacuum energy is calculable within any theory of

elementary particles, such as the Standard Model of particle physics, and the observed vacuum energy is the sum of a classical energy and an enormous quantum energy

Taipei June 2014

𝜍𝑤𝑏𝑑 = 𝜇 + 𝑛4 4𝜌 2

  • So what? Can always choose classical 𝜇 to ensure the

Universe accelerates by the right amount, even if 𝜍𝑤𝑏𝑑 is much smaller than 𝑛4

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SLIDE 61

Hierarchy problems

  • The electroweak hierarchy
  • The cosmological constant

Taipei June 2014

𝑀𝑇𝑁 = 𝜈20 + 𝑛2

0 𝐼∗𝐼 + 𝑒𝑗𝑛𝑓𝑜𝑡𝑗𝑝𝑜𝑚𝑓𝑡𝑡

𝜈2 = 𝜈2

0 + ℎ𝑗𝑕ℎ𝑓𝑠 𝑝𝑠𝑒𝑓𝑠

me ~ 106 eV m  10-2 eV mw ~1011 eV m ~ 108 eV

Modern picture: no unique

‘classical’ theory; instead many ‘effective’ theories

𝜍𝑤𝑏𝑑 = 𝜇0 + 𝑙𝜑𝑛𝜑

4

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SLIDE 62

Hierarchy problems

  • The electroweak hierarchy
  • The cosmological constant

Taipei June 2014

𝑀𝑇𝑁 = 𝜈20 + 𝑛2

0 𝐼∗𝐼 + 𝑒𝑗𝑛𝑓𝑜𝑡𝑗𝑝𝑜𝑚𝑓𝑡𝑡

𝜈2 = 𝜈2

0 + ℎ𝑗𝑕ℎ𝑓𝑠 𝑝𝑠𝑒𝑓𝑠

me ~ 106 eV m  10-2 eV mw ~1011 eV m ~ 108 eV

Modern picture: no unique

‘classical’ theory; instead many ‘effective’ theories 𝜍𝑤𝑏𝑑 = 𝜇1 + 𝑙𝑓𝑛𝑓

4 + 𝑙𝜉𝑛𝜉 4

𝜍𝑤𝑏𝑑 = 𝜇0 + 𝑙𝜉𝑛𝜉

4

slide-63
SLIDE 63

Hierarchy problems

  • The electroweak hierarchy
  • The cosmological constant

Taipei June 2014

𝑀𝑇𝑁 = 𝜈20 + 𝑛2

0 𝐼∗𝐼 + 𝑒𝑗𝑛𝑓𝑜𝑡𝑗𝑝𝑜𝑚𝑓𝑡𝑡

𝜈2 = 𝜈2

0 + ℎ𝑗𝑕ℎ𝑓𝑠 𝑝𝑠𝑒𝑓𝑠

me ~ 106 eV m  10-2 eV mw ~1011 eV m ~ 108 eV

Modern picture: no unique

‘classical’ theory; instead many ‘effective’ theories 𝜍𝑤𝑏𝑑 = 𝜇1 + 𝑙𝑓𝑛𝑓

4 + 𝑙𝜉𝑛𝜉 4

𝜍𝑤𝑏𝑑 = 𝜇0 + 𝑙𝜉𝑛𝜉

4

Must cancel to 32 decimal places!!

slide-64
SLIDE 64

What We’re Looking For

  • Our picture of the physics of ordinary particles must already

be wrong at energies higher than 1 eV, or distances shorter than 1 micron.

  • Whatever the change is, it must change gravity in such a

way as to produce a small response to the vacuum energy.

  • It must not alter other interactions.
  • Is this possible? Party line says “no”.

Taipei June 2014

slide-65
SLIDE 65

What We’re Looking For

  • Our picture of the physics of ordinary particles must already

be wrong at energies higher than 1 eV, or distances shorter than 1 micron.

  • Whatever the change is, it must change gravity in such a

way as to produce a small response to the vacuum energy.

  • It must not alter other interactions.
  • Is this possible? Party line says “no”.
  • Remarkably, it may be!

Taipei June 2014

slide-66
SLIDE 66

Helpful extra dimensions

Taipei June 2014

  • The Problem:
  • Einstein’s equations make a lorentz-invariant vacuum

energy (which is generically large) an obstruction to a close-to-flat spacetime (which we see around us)

𝑈

𝜈𝜉 = 𝜇 𝑕𝜈𝜉

𝐻𝜈𝜉 = 8𝜌𝐻 𝑈

𝜈𝜉

slide-67
SLIDE 67

Helpful extra dimensions

Taipei June 2014

  • The Problem:
  • Einstein’s equations make a lorentz-invariant vacuum

energy (which is generically large) an obstruction to a close-to-flat spacetime (which we see around us)

𝑈

𝜈𝜉 = 𝜇 𝑕𝜈𝜉

𝐻𝜈𝜉 = 8𝜌𝐻 𝑈

𝜈𝜉

Arkani-Hamed et al Kachru et al Carroll & Guica Aghababaie et al

But this need not be true if there are more than 4 dimensions!!

slide-68
SLIDE 68

Helpful extra dimensions

Taipei June 2014

  • Why not?
  • Extra dimensions need not be lorentz invariant
  • Vacuum energy might curve extra dimensions, rather

than the ones we see in cosmology

Vilenkin et al e.g. gravitational field of a cosmic string

slide-69
SLIDE 69

Helpful extra dimensions

Taipei June 2014

  • A higher-dimensional analog:
  • Similar (classical) examples also with a 4D brane in

two extra dimensions: e.g. the rugby ball and related solutions

Carroll & Guica Aghababaie et al

slide-70
SLIDE 70

Opportunities & Concerns

Taipei June 2014

  • If true, many striking implications:
  • Micron deviations from inverse square law
  • Missing energy at the LHC and in astrophysics:

requires Mg > 10 TeV

  • Probably a vanilla SM Higgs
  • Excited string states (or QG) at LHC below 10 TeV
  • Low energy SUSY without the MSSM
  • Very light Brans-Dicke-like scalars
  • Sterile neutrinos from the bulk?
slide-71
SLIDE 71

Taipei June 2014

“…when you have eliminated the impossible, whatever remains, however improbable, must be the truth.”

  • A. Conan Doyle
slide-72
SLIDE 72

Outlook

  • Cosmological observations are now redundantly testing

the Hot Big Bang model.

  • Observations support the ‘Concordance Cosmology’.

Taipei June 2014

slide-73
SLIDE 73

Outlook

  • Cosmological observations are now redundantly testing

the Hot Big Bang model.

  • Observations support the ‘Concordance Cosmology’.
  • The concordance involves several lines of independent

evidence for both Dark Matter and Dark Energy.

  • Neither can be dark forms of ordinary atoms.

Taipei June 2014

slide-74
SLIDE 74

Outlook

  • Cosmological observations are now redundantly testing

the Hot Big Bang model.

  • Observations support the ‘Concordance Cosmology’.
  • The concordance involves several lines of independent

evidence for both Dark Matter and Dark Energy.

  • Neither can be dark forms of ordinary atoms.
  • Dark Matter likely new particle types, but Dark Energy

is harder (until recently thought impossible).

  • If so we’ll know from a variety of observational tests.

Taipei June 2014