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Page 1: The State of the Universe

The State of the UniverseDavid Weinberg, Ohio State University

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The State of the Universe (as we know it)David Weinberg, Ohio State University

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The State of the Universe (as we think we know it)David Weinberg, Ohio State University

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Bottom Line

A wide range of current data are well explained by a cosmological model with

• A spatially flat Universe

• Dominated by cold dark matter and a cosmological constant

• ≈ 0.75, m ≈ 0.25, b ≈ 0.05, H0 ≈ 70 km s-1 Mpc-1

• Gaussian, adiabatic, primordial fluctuations that are

approximately (but not perfectly) scale-invariant.

Ongoing/planned experiments will substantially improve the

precision of cosmological tests and could poke holes in this picture.

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How Far We’ve ComeIn the mid-’80s, the main data to be explained were:

• galaxy clustering

• properties of galaxies

• existence of high-redshift quasars

• upper limits on CMB anisotropy

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How Far We’ve ComeToday: We argue about the parameters of flat inflationary cold dark matter models.

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The Path to CDM• COBE: Gravitational instability is right, inflation OK.

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The Path to CDM• COBE: Gravitational instability is right, inflation OK.

• Improving galaxy clustering and H0 data: harder to accommodate with m=1.

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The Path to CDM• COBE: Gravitational instability is right, inflation OK.

• Improving galaxy clustering and H0 data: harder to accommodate with m=1.

• Ly forest: Explains phenomenon not designed to explain.

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The Path to CDM

• COBE: Gravitational instability is right, inflation OK.

• Improving galaxy clustering and H0 data: harder to accommodate with m=1.

• Ly forest: Explains phenomenon not designed to explain.

• Type Ia supernova Hubble diagram: direct evidence for cosmic acceleration.

Riess et al. 1998

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The Path to CDM

• COBE: Gravitational instability is right, inflation OK.

• Improving galaxy clustering and H0 data: harder to accommodate with m=1.

• Ly forest: Explains phenomenon not designed to explain.

• Type Ia supernova Hubble diagram: direct evidence for cosmic acceleration.

• BOOMERANG/MAXIMA: Flat universe, clear acoustic peak. Strengthens supernova evidence for dark energy.

Jaffe et al. 2001

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Developments since 2000

• Substantial improvements in precision and dynamic range of measurements (WMAP, DASI, CBI, ACBAR; 2dFGRS, SDSS; larger and more distant supernova samples; precise Ly forest measurements)

• Addition of: Weak lensing, CMB polarization, CMB/BBN consistency on b.

• “Vanilla” CDM, with tot=1, w=-1, free parameters m, b, h, ns, As, looks close to consistent with all current data, though some tension on parameter values.

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Dark Matter• The Silver Bullet Cluster: qualitatively new evidence for dark matter vs. modified gravity.

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Clowe et al. 2006; fig. courtesy Doug Clowe

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Dark Matter• The Silver Bullet Cluster: qualitatively new evidence for dark matter vs. modified gravity.

• Small scale problems of cold dark matter:

• Excess of small scale structure (satellite galaxies).

• Wrong rotation profiles of disk galaxies.

My take: The case that these problems are related to dark matter not baryonic physics isn’t strong enough, and probably won’t become so.

• Ly forest lower limit on dark matter particle mass: 2.5 keV for thermal equilibrium decoupling, 14 keV for sterile neutrino (95% confidence; Seljak, McDonald, & Trac 2006)

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Seljak, Mcdonald, & Trac 2006 (astro-ph/0602430)

Ly forest flux power spectrum: cold dark matter vs. 6.5 keV sterile neutrino

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WMAP

Spergel et al. 2006 l ≈ 100 degs /

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WMAP

Spergel et al. 2006

3-yr data vs 1-yr data:

Smaller error bars throughout.

Key difference is new polarization measurement, changing central value and error bar on optical depth.

Changes central values on m

and 8: a lighter, less clustered universe.

Substantially reduces degeneracies among cosmological parameters.

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WMAP + SDSS LRGs

Tegmark, Eisenstein et al. 2006

SDSS adds turnover scale, tilt, and acoustic oscillation scale measured in km/s at z ~ 0.35.

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WMAP + SDSS LRGs

Tegmark, Eisenstein et al. 2006

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WMAP + SDSS LRGs

Tegmark, Eisenstein et al. 2006

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WMAP + SDSS LRGs

Tegmark, Eisenstein et al. 2006

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Supernova Hubble Diagram

Riess et al. 2004

Astier et al. 2006

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Supernova Hubble Diagram + SDSS BAO Scale

Astier et al. 2006

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Developments since 2000

• Substantial improvements in precision and dynamic range of measurements (WMAP, DASI, CBI, ACBAR; 2dFGRS, SDSS; larger and more distant supernova samples; precise Ly forest measurements)

• Addition of: Weak lensing, CMB polarization, CMB/BBN consistency on b.

• “Vanilla” CDM, with tot=1, w=-1, free parameters m, b, h, ns, As, looks close to consistent with all current data, though some tension on parameter values.

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Game Over?

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Game Over?The tyranny of vanilla:

Will we be cursed by a successful standard model with key elements that we don’t understand?

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Game Over?

Things we might find with improved data: • w = -0.9• w = -1.1• dw/dz|0.5 = 1, or (z=10) = 0.1.

• Inconsistency of gravitational and distance constraints on w: modified gravity, not dark energy.• tot = 1.02

• r = 0.1 (gravity waves), dns / d ln k = -0.03

• Primordial fluctuations have non-Gaussian or isocurvature component

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Future Experiments

Improved measurements of supernovae, weak lensing, galaxy clustering/baryon oscillations, Ly forest, CMB temperature and polarization anisotropies

An incomplete list:Current: SDSS-II, CFHT Legacy SurveyNear Future: PAN-STARRS, Planck, South Pole TelescopeMedium Term: Dark Energy Survey, SDSS-IIILong Term: LSST, Square Kilometer Array, JDEM, CMBPOL

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Bottom Line

A wide range of current data are well explained by a cosmological model with

• A spatially flat Universe

• Dominated by cold dark matter and a cosmological constant

• ≈ 0.75, m ≈ 0.25, b ≈ 0.05, H0 ≈ 70 km s-1 Mpc-1

• Gaussian, adiabatic, primordial fluctuations that are

approximately (but not perfectly) scale-invariant.

Ongoing/planned experiments will substantially improve the

precision of cosmological tests and could poke holes in this picture.