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Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Au stin Dark Energy Meeting@Ringb erg February 27, 2006

Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

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Page 1: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

Constraints on Dark Energy from CMB

Eiichiro Komatsu

University of Texas at Austin

Dark Energy Meeting@Ringberg

February 27, 2006

Page 2: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

Can CMB Constrain the Nature of Dark Energy?

• Which DE? Early Dark Energy (Inflaton Field) Intermediate Dark Energy (Tracker Field) Late Dark Energy

• Prospects for constraining the nature of DE with CMB ONLY is… Not so good for Early DE, if B-mode pol. is not detected. Not so good for Intermediate DE Not so good for Late DE

• Combination of CMB, LSS & SN is very powerful for constraining all of them (and everyone knows that), but let me try to talk just about CMB for 45 minutes (not so easy these days).

Page 3: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

What Can CMB Measure?• Baryon-to-photon ratio

Sound speed and inertia of baryon-photon fluid

• Matter-to-radiation ratio Matter-radiation equality “Radiation” may include photons, neutrinos as well as any other

relativistic components.

• Angular diameter distance to decoupling surface Peak position in l space ~ (Sound horizon)/(Angular Diameter

Distance)

• Time dependence of gravitational potential Integrated Sachs-Wolfe Effect

• Primordial power spectrum (Scalar+Tensor)

• Optical depth

Page 4: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

What CMB MeasuresA

mpl

itud

e of

tem

pera

ture

flu

ctua

tion

s at

a g

iven

sca

le, l

400 80020040 10010Multipole moment l~ Small scalesLarge scales

Ang.Diam. Distance

Baryon-to-photon Ratio

Mat-to-Radiation Ratio

ISW

Page 5: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

CMB to Parameters

Page 6: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

Matter-Radiation Ratio

• More extra radiation component means that the equality happens later.

• Since gravitational potential decays during the radiation era (free-fall time scale is longer than the expansion time scale during the radiation era), ISW effect increases anisotropy at around the Horizon size at the equality.

Page 7: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

Matter, , or Q?

Page 8: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

Angular Diameter Distance

dA=constant

Page 9: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

Error in dA = Error in rs

A

rs

dA

Page 10: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

ISW Effect

Therefore, one might hope that the ISW would help to break degeneracy between w and the other parameters. However…

w=-2

w=-0.6Weller & Lewis (2003)

Page 11: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

Perturbations in DE• Dark energy is required to be uniform in space (I.e., no fluctuations) if it

is a cosmological constant (w=-1).

• However, in general dark energy can fluctuate and cluster on large scales when w is not -1.

• The clustering of DE can… source the growth of potential, compensate the suppression of growth due to a faster expansion rate, and lower the ISW effect.

Weller & Lewis (2003)

•This property makes it absolutely impossible to constraint w with CMB alone, no matter how good the CMB data would be.

Page 12: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

CMB-LSS Correlation

• The same gravitational potential would cause ISW and LSS. Cross-correlation signal is an important cross-check of the existence of dark energy. There are ~2-sigma detections of various correlations: Boughn and Crittenden (2004): WMAP x Radio & X-ray sour

ces Nolta et al. (2004): WMAP x NVSS radio sources Scranton et al. (2003): WMAP x LRGs in SDSS Afshordi et al. (2004): WMAP x 2MASS galaxies

• But it’s hard! CMB is already signal-dominated on large scales, so nothing

to be improved on the CMB side. An all-sky galaxy survey observing 10 million galaxies at 0<z

<1 gives only 5-sigma detection (Afshordi 2004).

Page 13: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

CMB-WL Correlation

• Non-linear growth of structure at small scales also provides the ISW signal (a.k.a. RS effect)

• Would that be observable (ever)? The future lensing experiments would be signal-dominated. A lot of room for CMB experiments to improve at small scal

es.

RS

Page 14: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

• The RS-WL correlation picks up a time-derivative of the growth rate of structure: a sensitive measure of w

• Several different source redshifts allow us to do tomography on the time derivatives.

Page 15: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

RS-WL Correlation: Prediction

Nishizawa & Komatsu (in prep.)

Positive Correlation (ISW)

Negative Correlation (RS)

Assumed CMB experiment: 100deg2, 1 arcmin resolution, 1uK noise per pixel

High S/N!

Page 16: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006

Summary• CMB constraints DE properties via

Matter-to-radiation Ratio (useful for constraining Tracker field)

Angular Diameter Distance (degeneracy lines in w-h and w-Omega)

ISW (not very useful)

• Massive degeneracy between w and h and matter density makes it absolutely impossible for CMB alone to constrain DE properties. It does not matter how good the CMB data would be. It is essential to combine it with LSS and/or SNe.

• CMB-WL correlation may serve as an additional test of DE properties. Future small-scale CMB experiments might want to increas

e their angular resolution to ~1 arcmin level.

Page 17: Constraints on Dark Energy from CMB Eiichiro Komatsu University of Texas at Austin Dark Energy Meeting@Ringberg February 27, 2006