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Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

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Page 1: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Dark Energy

Bengt Gustafsson: Current problems in Astrophysics

Lecture 3 Ångström Laboratory, Spring 2010

Page 2: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Reading:

Frieman, Turner, Huterer: Dark Energy and the Accelerating Universe, Ann Rev. Astron. &

Astrophys 2008. 46-385

Page 3: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Friedmann equations:

• H2 = (a’/a)2 = 8G/3 - k/a + /3• a”/a = -4G/3 ( + 3p) + /3Einstein (1917). Zeldowich (1968):

wi = pi/i

wv = -1

= 8Gv = - 8Gpv

Estimated value gets very big. ”Cosmological constant problem”!

Page 4: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010
Page 5: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Among astronomers in the 80’s and 90’s: growing uneasiness with =

0.

• Globular clusters older than Hubble age• Large scale structure simulations• Statistics of lensed quasars

Page 6: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Discovery 1998: SN Ia

studies• Possible due to demonstration that SNe Ia are useful as ”standard candles” (Phillips 1993)

• -> Chandrasekhar mass 1.4 Msun.

-> 0.6 Msun of 56Ni, radioactive

decacy determines peak luminosity.

AND due to mosaics of CCD:s in cameras

on 4m class telescopes. Searches for supernovae scheduled.To determine cosmic deceleration!

QuickTime™ and a decompressor

are needed to see this picture.

Page 7: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Riess et al.,

Perlmutter et al.

Page 8: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Critique: Peak luminosity

metallicity (age) dependent?

Dust content or properties varying with metallicity?

Selection bias in low-z sample?

Page 9: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Futher evidence

- Cosmic Microwave Background- Large Scale Structure:

– Baryonic acoustic oscillations– Integrated Sachs-Wolfe Effect– Weak gravitational lensing

-X-ray clusters (requiring f = b/dm not to vary with z)

Page 10: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Millenium simulation

QuickTime™ and a decompressor

are needed to see this picture.

Millenium simulation (1010 particles)(Springel, White, Jenkins et al.)

Page 11: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

• FIG 8

Page 12: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

WHAT IS IT?

• Cosmological constant? No further insight• Vacuum energy? v ~ ∑fields gi kmax

4

Cutoff at Planck scale (1019 GeV) => x10120 too much! Even electron mass scale => U absurd!

SUSY: gi = +1 for bosons, -1 for fermions No perfect symmetry though, if broken at ~ 1TeV => x1060

If vacuum energy scale randomly varying and somewhere very low, we would live there (Weinberg 1987). Anthropic explanation?

Page 13: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

What is it?, cont.

Scalar fields? Opens up more possibilities. May clump?May relate to inflation? Does not solve v problem. w≠-1. May vary with a(z).

Modified gravity? Interesting ideas, no self-consistent theory in agreement with LSS and CMB results yet.

Inhomogeneities?Kolb et al. Enough??

Page 14: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

Near (?) future: More observations!

• Supernovae• Galaxy clusters• Baryonic Acoustic Oscillations• Weak gravitational lensing

From Frieman et al. (2008)

Page 15: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

WHAT WE KNOW NOW:

• Strong evidences for accelerated expansion

• Dark energy a probable cause• Vacuum energy problematic

= 0.76±0.02, w ≈ -1.0 ±0.1(stat) ±0.1 (syst) if w constant.

Assuming w=w0 + wa(1-a):

= 0.70±0.15, w0 ≈ -1.0 ±0. 2, wa = 0±1.

Page 16: Dark Energy Bengt Gustafsson: Current problems in Astrophysics Lecture 3 Ångström Laboratory, Spring 2010

MAJOR QUESTIONS NOW

• Is dark energy something else than vacuum energy?

• Does GR selfconsistently describe cosmic acceleration and structure formation?