how can cmb help constraining dark energy? licia verde icrea & institute of space sciences (ice...
TRANSCRIPT
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
How can CMB help constraining dark energy?
Licia VerdeICREA & Institute of space Sciences (ICE CSIC-IIEC)
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.QuickTime™ and a
TIFF (Uncompressed) decompressorare needed to see this picture.
QuickTime™ and aTIFF (Uncompressed) decompressorare needed to see this picture.
Interpretation key:
Black background: background material/work by others
White background: work I am directly involved with/my biased view
The standard cosmological model
Spatially flat Universe QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Power-law, primordial power spectrum
Only 6 parameters: WMAP5yr analysis
CDM model
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Survived 15 years of data!
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Dark energy from CMB
2dfGRS
H prior
WMAPII
SN
With DE clusteringWMAP3
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Dark energy
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
WMAP5
Komatsu et al (2008)
Why so weak dark energy constraints from CMB?
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
WMAP5
Dunkley et al (2008)
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
If I wanted to reconstruct non parametrically V
Theoretical physicists: which parameterization?
To give you a flavor, assume it is a slowly rolling potential and think about inflation
Similar to horizon flow parameters (from Simon et al 2005; Fernandez-Martinez & LV ‘08)
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
H(z)
H(z)
Just integrate to get(z)
You need to have a parameterization (or a model)QuickTime™ and a
TIFF (LZW) decompressorare needed to see this picture.
Can be integrated analytically!
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
No single observation that I know of can give this
Why so weak dark energy constraints from CMB?
The limitation of the CMB in constraining dark energy is that the CMB is located at z=1090.
We need to look at the expansion history (I.e. more than one snapshot of the Universe)
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
WMAP5Dunkley et al (2008)
Several options….
THE SYMPTOMSOr OBSERVATIONAL EFFECTS of DARK ENERGY
Recession velocity vs brightness of standard candles: dL(z)
CMB acoustic peaks: Da to last scattering
LSS: perturbations amplitude today, to be compared with CMB
Da to zsurvey
Perturbation amplitude at zsurvey
Leading observational techniques to go after dark energy
Supernovae
Baryonic Acoustic Oscillations (BAO)
Weak Lensing
Galaxy clusters number counts
(expansion history)
(expansion history)
(growth of structure and expansion history)
(mostly growth of structure)
Q: A combination of techniques will be best for at least two reasons
What if one could see the peaks pattern also at lower redshifts?
weak dark energy constraints from CMB?
BUT The CMB encloses information about the growth of foreground structures: secondary CMB!
Integrated Sachs Wolfe effect
Secondary effects: Sunyaev Zeldovich(SZ), Kintetic SZ, Rees-Sciama, Lensing.
A
B
C … resort to other probes
(and get other things for free)
C … resort to other probes
Take the “concordance approach”
CMB offers an anchor point at a time where Dark energy is unimportant
..or is it?
Acquaviva & LV 2007 considered a Brans-Dickie model,which looks like L at late times and which has virtually the same Growth of structure as LCDM
Example: If you try to “hide” Dark Energy…
Still shows up in the concordance approach….
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
What if one could see the peaks pattern also at lower redshifts?
weak dark energy constraints from CMB?
BUT The CMB encloses information about the growth of foreground structures: secondary CMB!
Integrated Sachs Wolfe effect
Secondary effects: Sunyaev Zeldovich(SZ), Kintetic SZ, Rees-Sciama, Lensing. (cross correlations!)
A
B
C … resort to other probes
(and get other things for free)
USE the CMB as BACKLIGHT, illuminating the foreground universe
High z mid z low z
• First galaxies • Universe is reionized• Ostriker-Vishniac• Diffuse thermal SZ
• Cluster formation: Sunyaev-Zel’dovich (SZ)• Kinematic SZ• Lensing of the CMB
• The growth of structure is sensitive to dark energy• Rich additional science from correlations among effects
• Extraction of cosmological parameters• Initial conditions for structure formation
Sunyaev-Zel’dovich (SZ) clusters
e-
e-
e-
e-
e-
e-
e-
e-
e-
Coma Cluster Telectron = 108 K
Optical: Redshift and Mass
mm-Wave: SZ –Compton Scattering
X-ray Flux: Mass
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
http://www.physics.princeton.edu/act/
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
Barcelona, Cardiff, Columbia, Haverford, Inaoe, KwaZulu-Natal, NASA, NIST,UPenn,Princeton, U. Pittsburgh, Rutgers, Toronto, UBC, Cape Town, Universidad Catolica, York College
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
The south pole telescope
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
http://pole.uchicago.edu/public/ QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
19
Kinetic SZ/Ostriker-Vishniac (OV)
Non-Gaussian but with CMB frequency spectrum. Spatially distinguishable. Requires a high fidelity map.
Amplitude of OV signal determines epoch of reionization.
OV power spectrum measures the density and velocity fluctuations at reionization.
Bulk velocity of HOT electrons from ionization by the first stars (OV) or in clusters and filaments (KSZ).
ve
Bulk Velocity of hot electrons.
CMB photon
KSZ measures cluster bulk velocity field at low z.
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
Velocities: using the KSZ signal
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
W=-1.0
W=-0.6
(Hernandez-Monteagudo, LV, Jimenez, Spergel 2006)
The peculiar velocity field is sensitive to the onset of the late acceleration of the Universe.
Recall that KSZQuickTime™ and a
TIFF (Uncompressed) decompressorare needed to see this picture.
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
Narrow and deep
Wide and shallow
...++Δ
+Θ∇•Δ
+Δ
≅Δ
SZTT
TT
TT
TT NLPP
γ
Lensing
∫ Φ−
−=Θ*
0 *
* ),(2)(r
drrrrr
rrγγ
drrrtT
T NLNL
),(2 γΦ∂∂
=Δ
∫
Rees-Sciama
Low z(high l )
High z (low l )
Depends on w,0Ω
Gravitational potential
Lensing and Rees-SciamaLensing and Rees-Sciama(LV, Spergel 2002)
ISW, but non-linear
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Bispectrum :
to couple the high z universe (low ) to the low z universe (high ) via the weak lensing signal
Balance of 2 competing contributions:
=>Decay of gravitational potential (non Einstein de Sitter Universe)
=>Amplification due to non-linear gravitational evolution
Balance depends on Ωm and w
321
3
3
2
2
1
1
321
321
321
321lllllllll
lllB
mmmaaaB mmmmmm
⎟⎟⎠
⎞⎜⎜⎝
⎛==
ll
Consider primordial, lensing & Rees-Sciama:
(Verde, Spergel 2002)
Bispectrum: Cross correlating primordial-lensing-Rees Sciama
Forecast: ACT+WMAP data
Fiducial model
See also Giovi Baccigalupi, Perrotta 2004 for w(z)
What if one could see the peaks pattern also at lower redshifts?
weak dark energy constraints from CMB?
BUT The CMB encloses information about the growth of foreground structures: secondary CMB
Integrated Sachs Wolfe effect
Secondary effects: Sunyaev Zeldovich(SZ), Kintetic SZ, Rees-Sciama, Lensing.
A
B
C … resort to other probes
(and get other things for free)
Investment portfolio
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Investment portfolio
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Low risk investment
Medium risk, medium gain
High risk, high potential for return
Cosmic clocks: with D. Stern, M. Kamionkowski, R. Jimenez,T. Treu
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.QuickTime™ and a
TIFF (LZW) decompressorare needed to see this picture.
+GDDS
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
- - -WMAP3+SDSS+HST
+H(z)
GDDS +high z radiogalaxies + Treu et al. 2000 sample
From Simon, Verde, Jimenez (2005)
After tornado, earthquakes, tsunami warnings and fires…. we got data! Watch this space…
Simon et al 05Assumes Flatness
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Fernandez-Martinez & LV 08Relaxing priors including flatness
Forecast: need ~1000 high resolution spectra
2 measurements in one?
Challenge: scale of interest ~100 Mpc/h: large volumes!
Feature: measure BOTH dA and H(z) from 3D clustering
Line of sight (radial)
Plane of the sky (angular)
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Pau collaboration. (2008)
Spectroscopy or photometry?
AAOmega
600K galaxies, z~1 (10% error on w)
WFMOS several million galaxies >2012
VISTA, DES, LSST
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.Degrade information in the z direction but is faster & can cover more sky
The debate is still open!
Could do weak lensing almost for free
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
PAU: Physics of the Accelerating Universe
Awarded consolider-ingenio 2010, E. Fernandez, PI
Survey ~10000 deg2 0.1<z<1.0, ~14M LRG galaxies, 100’s M total
“Hybrid” technique: narrow band photometry (the best of both worlds?)
Likely: dedicated telescope. New camera (~40 narrow band filters)
Instituto de fisica de alta energias (IFAE-Barcelona)Instituto de ciencias del Espacio (ICE-Barcelona)Instituto astrofisico de Andalucia (IAA-Granada)Instituto de fisica teorica (IFT-Madrid)Centro de investigaciones[…] (CIEMAT-Madrid)Instituto de fisica corpuscolar (IFIC -Valencia)Puerto de informacion Cientifica(PIC-Barcelona)
Close collaboration between particle physicists (theorists and experimentalists) and astrophysicists (theorists and observers)
Measures both H(z) and Da(z)
http://www.ice.csic.es/research/PAU/PAU-welcome.html
goal
goal
goal
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Bruzual & Charlot11 Gyr @ z=0.2
THE IDEA:
New photometric system
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Courtesy of A. Fernandez-Soto
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
ALHAMBRA
Courtesy of A. Fernandez-Soto
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Bruzual & Charlot11 Gyr @ z=0.2
THE IDEA:
New photometric system
What filters? How?
Redshift error degradation
Feature width~15Mpc (comoving)QuickTime™ and a
TIFF (LZW) decompressorare needed to see this picture.
Radial direction H(z) Plane of sky direction Da
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
1M halos,
M>3.7d13Msol
MICE simulation
27 (Gpc/h)^3
PAU collab. 2008
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
+ other science: galaxy formation and evolution, accurate measurement of P(k) and growth through higher-order correlations, primordial non gaussianity, metalicity for halo stars), etc…
A mine of information for studying galaxy formation!
Example: Clustering of peaks (DM halos) of a non-gaussian density field
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Dalal et al 08; Matarrese, Verde 2008
fNL=100
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
General non-gaussianity
ΦxxfNLxxIF as motivated by inflation, then
Summary: Much ado about nothing
Observations indicate that nothing weighs something (but much less than expected) and make the universe accelerate (other options are still Possible, inhomogeneities, gravity, but the result must “look like ”).
Heroic observational effort is on going(we’ll learn not only about dark energy from it)
We HAVE TO ask: “how interesting it is really to add yet another significant figure to or w ?”
What would it take to discriminate?discuss
discuss
My personal view: The answer lies in the interface between Astronomy and Theoretical physics, if we take the“Accelerating universe challenge”, there is no other way.
The standard cosmological model is extremely successful, but….
QuickTime™ and aTIFF (LZW) decompressor
are needed to see this picture.
Challenges of the accelerating universe:Zero-th order challenge: create a new culture of particlephysicists and astronomers working together, theorists and experimentalists
First_order challenge: If it is why is it so small? On this issue astronomers have done their work already (I.e. is non zero)Now it is the job of theoretical physicists.
Second order challenge: is it dynamical? and if so how does it evolve?
Third order challenge: “could we have been wrong all along?”did Einstein had the last word on gravity? Or FRW on the metric?
The data challenge: Avalanche of data coming soon The systematics challenge: systematic errors in many cases will be the limit
“In the middle of difficulty lies opportunity" --- A. Einstein