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Constraints on Dark Energy from CMB

Eiichiro Komatsu

University of Texas at Austin Dark Energy Meeting@Ringberg

February 27, 2006

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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 constrai

ning all of them (and everyone knows that), but let me try to

talk just about CMB for 45 minutes (not so easy these days).

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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

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What CMB Measures

mplitude of temperature fluctuations at a given scale, l

400 800

200 40 100

10

Multipole moment

l~

Small scales Large scales

Ang.Diam. Distance

Baryon-to- photon

Ratio

Mat-to- Radiatio n Ratio

ISW

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CMB to Parameters

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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.

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Matter, , or Q?

(8)

Angular Diameter Distance

d

A

=constant

(9)

Error in d A = Error in r s

A

r s

d A

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ISW Effect

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

However…

w=-2

w=-0.6

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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.

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CMB-LSS Correlation

• The same gravitational potential would cause ISW and L SS. Cross-correlation signal is an important cross-check of the existence of dark energy. There are ~2-sigma det ections of various correlations:

Boughn and Crittenden (2004): WMAP x Radio & X-ray source s

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).

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CMB-WL Correlation

• Non-linear growth of structure at small scales also provi des 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 scales.

RS

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

• Several different source redshifts allow us to do tomography on th

e time derivatives.

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RS-WL Correlation: Prediction

Nishizawa & Komatsu (in prep.)

Positive Correlation (ISW)

Negative Correlation (RS)

Assumed CMB experiment: 100deg

2

, 1 arcmin resolution, 1uK noise per pixel

High S/N!

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Summary

• CMB constraints DE properties via

Matter-to-radiation Ratio (useful for constraining Tracker fie ld)

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

ISW (not very useful)

• Massive degeneracy between w and h and matter de nsity makes it absolutely impossible for CMB alone t o 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.

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