+ All Categories
Home > Documents > Lecture 3: Modified matter models of dark energy

Lecture 3: Modified matter models of dark energy

Date post: 13-Jan-2016
Category:
Upload: montana
View: 28 times
Download: 1 times
Share this document with a friend
Description:
Lecture 3: Modified matter models of dark energy. Shinji Tsujikawa (Tokyo University of Science). What is the origin of dark energy?. The simplest candidate: Cosmological constant. However this suffers from a fine-tuning problem if it originates from a vacuum energy. - PowerPoint PPT Presentation
Popular Tags:
29
Lecture 3: Modified matter models of dark energy Shinji Tsujikawa (Tokyo University of Science)
Transcript
Page 1: Lecture 3: Modified matter models of dark energy

Lecture 3:Modified matter models of dark energy

Shinji Tsujikawa(Tokyo University of Science)

Page 2: Lecture 3: Modified matter models of dark energy

What is the origin of dark energy?

The simplest candidate: Cosmological constant However this suffers from a fine-tuning problem

if it originates from a vacuum energy.

Dynamical dark energy models

Quintessence, k-essence, chaplygin gas, tachyon, f (R) gravity, scalar-tensor theories, Braneworld, Galileon, …

Page 3: Lecture 3: Modified matter models of dark energy

Cosmological constant:

Λ Originally introduced by Einstein to realize the static Universe .

1917 (38 old) 1945 (66 old)

‘Biggest Blunder in my life’

1998 (119 old:heaven)

In 1929Hubble found the expansion of the Universe.

Static Universe

Big Bang Cosmology

Big Bang cosmology+cosmic acceleration

Page 4: Lecture 3: Modified matter models of dark energy

Cosmological constant problem

The energy scale of dark energy today is

or, Cosmo-illogical constant problem (by Rocky Kolb)

If we take the Planck scale as a cut-off scale, the energy scale of the vacuum energy is

Problem even before 1998

See my review in 1989. by Steven Weinberg

Page 5: Lecture 3: Modified matter models of dark energy

The cosmological constant is (i) sufficiently small to explain the energy scale of dark energy?(ii) or, completely zero?

Case (i): Both the cosmological constant and the dark energy problems are solved at the same time.

Economical

Case (ii): The cosmological constant problem is solved, but the      dark energy problem has to be addressed.

This possibility remains.

`Modified matter’ (such as a scalar field) is introduced, or gravity is modified from Einstein gravity (Dynamical dark energy) .

Page 6: Lecture 3: Modified matter models of dark energy

Example of case (i): de-Sitter vacua in string theory

Kachru-Kallosh-Linde-Trivedi (KKLT) scenario

Type II string theory compactified on a Calabi Yau manifold with a flux.

The KKLT scenario consists of three steps.

Potential: where

Page 7: Lecture 3: Modified matter models of dark energy

We add uplifting potential generated by anti-D3 braneat the tip of warped throat:

uplifting

It is possible to explain dark energy if

The total potential is

AdS

dS

Page 8: Lecture 3: Modified matter models of dark energy

String Landscape

We may live in a vacuum with a small energy density (related with anthropic selection).

10 upliftedvacua!

500

Page 9: Lecture 3: Modified matter models of dark energy

Example of case (ii) [vanishing cosmological constant]

_________________ ______K: Kahler potentialW: Superpotential

In supersymmetric theories the vacuum energy is zero if supersymmetry is unbroken, but in real word supersymmetry is broken.

Cancellation is required

Page 10: Lecture 3: Modified matter models of dark energy

  

We can classify the models into two classes .

(i) Modified gravity (ii) Modified matter

f(R) gravity,Scalar-tensor theory,Braneworlds,Gauss-Bonnet gravity,Galileon gravity,…..

Quintessence,K-essence,Chaplygin gas,Coupled dark energy,(including mass varying neutrinos)…..

Dynamical dark energy models

(Einstein equation)

Page 11: Lecture 3: Modified matter models of dark energy

Modified matter models based on scalar fields

• Quintessence (‘fifth element’):

Chiba, Sugiyama, Nakamura (1997) ‘X matter’

Caldwell, Dave, Steinhardt (1998) ‘Quintessence’

• K-essence:

Accelerated expansion based on the potential energy

where

Chiba, Okabe, Yamaguchi (1999) ‘Kinetically driven quintessence’

Accelerated expansion based on the kinetic energy

Armendariz-Picon, Mukhanov, Steinhardt (2000) ‘k-essence’

Page 12: Lecture 3: Modified matter models of dark energy

Quintessence: French wine!

_____________________________

Page 13: Lecture 3: Modified matter models of dark energy

φφφφ

ÉXÉJÉâÅ[èÍÇÃÉ|ÉeÉìÉVÉÉÉãÉXÉJÉâÅ[èÍÇÃÉ|ÉeÉìÉVÉÉÉãÉXÉJÉâÅ[èÍÇÃÉ|ÉeÉìÉVÉÉÉãÉXÉJÉâÅ[èÍÇÃÉ|ÉeÉìÉVÉÉÉã

ÉtÉ@ÉìÉgÉÄÉNÉCÉìÉeÉbÉZÉìÉX

Potentials of Quintessence

As long as the potential is sufficiently flat, cosmic acceleration can be realized.

Energy density:

Pressure:

Equation of state for Quintessence

Quintessencephantom

Quintessence can be distinguishedfrom the LCDM.

Page 14: Lecture 3: Modified matter models of dark energy

Particle physics models of quintessence

(i) Fermion condensate in globally supersymmetric QCD theories (Binetruy)

The inverse power-law potential was derived.

where

(ii) Supergravity models (Brax and Martin, Copeland et al)

The field potential in SUGRA theories is

Page 15: Lecture 3: Modified matter models of dark energy

(iii) Pseudo-Nambu Goldston Boson (PNGB) models (Friemann et al)

The filed starts to evolve only recently.

Page 16: Lecture 3: Modified matter models of dark energy

Classification of Quintessence potentials (Caldwell and Linder, 2003)

(A) Freezing models:

Since the potential tends to be flatter, the evolutionof the field slows down.

(B) Thawing models:

The field has been nearly frozen in the past, but it starts to evolve around today

.

.Example

Example

Page 17: Lecture 3: Modified matter models of dark energy

Quintessence in the (w,w’) plane

.

LCDM

The current observations are not still enough tofind the evidence for the variation of the equation of state.

Page 18: Lecture 3: Modified matter models of dark energy

Dynamical system approach to quintessence

Page 19: Lecture 3: Modified matter models of dark energy

Dynamical equations

The fixed point responsible for the cosmic acceleration is

Page 20: Lecture 3: Modified matter models of dark energy

Phase space

Attractor(cosmic acceleration)

Saddle(matter point)

Page 21: Lecture 3: Modified matter models of dark energy

General potentials

where

(tracking condition)

Tracking always occurs.

Page 22: Lecture 3: Modified matter models of dark energy

Numerical simulations for

Page 23: Lecture 3: Modified matter models of dark energy

K-essenceK-essence is described by the action

where

The models that belong to k-essence is

Conformal transformation

or

Page 24: Lecture 3: Modified matter models of dark energy

Equation of state for k-essence

Page 25: Lecture 3: Modified matter models of dark energy

Stability condition for k-essence

Page 26: Lecture 3: Modified matter models of dark energy

Some people tried to solve the coincidence problem of dark energy by considering a specific Lagrangian

However it is difficult to construct such models theoretically. Moreover they typically have the superluminal propagation speed.

k-essence density parameter

Armendariz-Picon, Mukhanov, Steinhardt (2000)

Page 27: Lecture 3: Modified matter models of dark energy

Chaplygin gas model

Chaplygin gas Generalized Chaplygin gas

This corresponds to unified dark energy models in which darkmatter and dark energy are explained as a single component.

(pressureless matter)

(dark energy)

Continuity equation:

Page 28: Lecture 3: Modified matter models of dark energy

Past:

Future:

Page 29: Lecture 3: Modified matter models of dark energy

Chaplygin gas satisfies observational constrants ? No!

Matter power spectrum

_____________________

The sound speed term prevents the growth oflarge-scale structure.

Observational constraints

This cannot be distinguishedfrom the LCDM.


Recommended