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COMING HOME COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago
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COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

Dec 22, 2015

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Page 1: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

COMING HOMECOMING HOME

Michael S. Turner

Kavli Institute for Cosmological Physics

The University of Chicago

Page 2: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

Some Cosmological Some Cosmological Observations from AfarObservations from Afar

Page 3: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

No Chinks in “The No Chinks in “The New Cosmology”New Cosmology”

• WMAP + SDSS + 2dF + HST Key Project + DASI + ACBAR + CBI + t0 + SNe …

• Smaller error bars, consistency remains– σ(n): 0.1 to 0.02; σ(Ω0): 0.03 to 0.01; σ(w): 0.2 to

0.1

• Hubble constant has been constant for 5 years! H0 = 72 ± 7 km/s/Mpc

• Looking better than ever – almost ready for a real name!

(i.e., CDM + Dark Energy + Inflation)

Page 4: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

Precision Cosmology is Precision Cosmology is Harder than Theorists’ Harder than Theorists’

projectionsprojections

• “Bits & bites”

• l = 2 to 5

• Optical depth:

τ = 0.17 to 0.09

Page 5: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

Serious testing of Serious testing of Inflation has Inflation has begunbegun

Key Predictions1. Flat Universe2. Almost scale-invariant, Gaussian perturbations: |(n-1)| ~ 0.1 and |dn/dlnk| ~ 0.0011. Gravity waves: spectrum, but not amplitude predicted

Key Results1. Ω0 = 1.0 ± 0.012. (n-1) = 0.96 ± 0.017*; dn/dlnk = -0.1 ± 0.05; no

evidence for nonGaussianity3. r < 0.55 (95% cl)*

*Depends significantly upon the priors assumed

Page 6: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

Cosmic AccelerationCosmic AccelerationDark EnergyDark Energy

• Evidence for cosmic acceleration has gotten stronger (HST, CFHTLS, Essence, WMAP, XMM/Chandra…)

• Still no understanding – “theorists continue to explore phase space”

• No evidence that dark energy is not the energy of the quantum vacuum

– w = -1 ± 0.1 (from ± 0.2); no evidence for time variation

• Very significant probes on the horizon:– JDEM, LSST, …

Page 7: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.
Page 8: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

Loose EndsLoose Ends

1. Precision test (few percent) using baryon density: BBN (D/H) vs. CMB (odd/even) unrealized

2. Consistency of BBN light element predictions (He – D – Li tension)

3. σ8: lack of consistency4. Cosmic variation of α5. Excess power at l ~ 20006. “LSND 4th neutrino”7. DAMA, e+ excess, …

Page 9: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

What Do We Really Know What Do We Really Know About Cosmic AccelerationAbout Cosmic Acceleration

Charles A. Shapiro & Michael S. Turner,astro-ph/0512586

Page 10: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

Much of What We Know About Much of What We Know About Cosmic Acceleration Traces to Cosmic Acceleration Traces to

Model Assumptions (Model Assumptions (ΛΛCDM, wCDM)CDM, wCDM)

• ΛCDM, wCDM are much better fits than models w/o “dark energy” (CDM or OCDM)

• … but, the acceleration history is fixed: recent acceleration, past deceleration

• In addition, the correctness of Friedmann equation is assumed (what if gravity theory is part of the solution?)

Page 11: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

Assumptions & InputsAssumptions & Inputs

• Metric theory of gravity with Robertson-Walker metric

• “Friedmannless” analysis• Reiss et al’s Gold Set of Supernovae (adding

CFHT Legacy doesn’t change things much)• Flat Universe (can be relaxed – more later)• Piecewise constant acceleration histories• Principal component analysis for q(z)

Page 12: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.
Page 13: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

Robust ConclusionsRobust Conclusions

• Universe may not be accelerating today: Model with deceleration since z = 0.3 is acceptable at 10% cl

• Very strong evidence that Universe once accelerated (5σ) (from best determined mode)

• Strong evidence that q(z) was larger in the past (other well determined modes)

• Weak evidence that Universe decelerated in the past

Page 14: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

6 Most Well Determined Principal Components

Dec

eler

atio

n

Redshift

Page 15: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

ΛCDM

2 Best Determined Modes

Page 16: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

Without Friedmann Equation Best Without Friedmann Equation Best Evidence for Flatness is Lost Evidence for Flatness is Lost

(i.e., CMB Anisotropy)(i.e., CMB Anisotropy)

• Might be able to determine spatial curvature independently:

dV = r2drdΩ / [1 - kr2]1/2

r(z) = coordinate distance to object with redshift z|k|-1/2 = curvature radius

• Determine r and dr (e.g., SNe) and dV (e.g. number counts), infer k

Page 17: COMING HOME Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago.

My List of Burning IssuesMy List of Burning Issues

1. Cosmic Acceleration/Dark Energy: “Most Profound Mystery in all of Science”

2. Dark Matter: 3 pronged approach – space, accelerators, and underground expt’s – the prize is within sight!

3. Testing the predictions of inflation – inflation is knocking at the door to become part of “standard cosmology”

4. Using the consistency and crosschecks now afforded by precision cosmological data (BBN, SDSS/2dF, WMAP, SNe…) to test General Relativity in new regimes