a brief history of the cmb
TRANSCRIPT
April 2, 2015 Ganga/CMB & Planck 2
A Brief History of the CMBPenzias & Wilson
discovered it.
COBE Measured it.
WMAP Used it.
Planck Refines it.
April 1, 2015/Ganga Cosmological Parameters 3
Visualize the Evolution of the Universe
The microwave background light we see today was
created “just after” the Big Bang (~380k yr)
As such, it is a “baby picture” of the early Universe. By studying it, we hope to understand it's birth.
http://map.gsfc.nasa.gov/media/060915/index.html
April 2, 2015 Ganga/CMB & Planck 4
Many Different Effects Together
TT
EE
BB
Lensing GWB
max compressionmax rarefaction
photondiffusion
scale
reionization: peaklocation ~ (SLS horizon) x
sqrt(z_reion / z_rec) ~ 10
inflationpotential
curvature,acoustic horizon
baryon density
damping from photondiffusion, sensitive to
matter density
SLS thickness (~ 860)
Sachs-Wolfe effect
SLS horizonscale (~ 100)
oscillations out of phase:TT ~ density extrema,EE ~ velocity extremaoscillationfrequencydiffers by factorof sqrt(3): sound vs. light speed
gravitational waveson small scales decay away(amplitude ~ 1/a)
ratio of quadrupolemoment power = T/S( = 0.05 in this plot)
Cynthia Chiang
April 2, 2015 Ganga/CMB & Planck 5
IntroductionPrecursors COBRAS
and SAMBA
conceived in 1993.
Selected in 1996, with inputs from
failed WMAP
competitors FIRE and
PSIhttp://www.cosmos.esa.int/documents/387566/387653/Ferrara_Dec1_09h50_Bersanelli_Planck_mission.pdf
April 2, 2015 Ganga/CMB & Planck 6
IntroductionHFI
became polarization sensitive in
2001 (~when
WMAP was launched).
Planck was launched 14 May
2009. (~13 years from selection to
launch.)http://www.cosmos.esa.int/documents/387566/387653/Ferrara_Dec1_09h50_Bersanelli_Planck_mission.pdf
April 2, 2015 Ganga/CMB & Planck 7
LaunchPlanck was launched May 14, 2009 aboard an
Ariane 5 along with the Herschel Space Observatory, which is also orbiting around L2.
April 2, 2015 Ganga/CMB & Planck 8
Voyage and OrbitPlanck traveled the 1.5 million
kilometers to the second Sun-
Earth Lagrange point in about three months
April 2, 2015 Ganga/CMB & Planck 9
Planck's Orbit around L2Planck orbits around the
second Sun-Earth Lagrange point, about 1.5 million kmfurther from the Sun than
the Earth
A diagram from Wikipedia showing the Sun–Earth L2 point, which lies
well beyond the Moon's orbit around the Earth
April 2, 2015 Ganga/CMB & Planck 10
Planck's Scanning Strategy
Planck scans the sky in (almost)
great circles in a plane defined by the Sun-
Earth axis. The full sky is (almost) covered each six months.
April 2, 2015 Ganga/CMB & Planck 11
Frequency/wavelength coveragePlanck fills
the SubMM
range, so in addition
to CMB science,
Planck will be able to say a lot
about dust emission
in our Galaxy and in
others.
April 2, 2015 Ganga/CMB & Planck 12
Frequency/wavelength coveragePlanck fills
the SubMM
range, so in addition
to CMB science,
Planck will be able to say a lot
about dust emission
in our Galaxy and in
others.
April 2, 2015 Ganga/CMB & Planck 13
Frequency/wavelength coveragePlanck fills
the SubMM
range, so in addition
to CMB science,
Planck will be able to say a lot
about dust emission
in our Galaxy and in
others.
April 2, 2015 Ganga/CMB & Planck 14
Planck MapsPlanck has twoinstruments:
- LFI:-- 30,-- 44,-- 70 GHz
- HFI-- 100,-- 143,-- 217,-- 353,-- 545,-- 857 GHz
April 2, 2015 Ganga/CMB & Planck 15
Asteroids and Zodiacal Emission
April 1, 2015/Ganga Cosmological Parameters 16
The CMB and Galactic Dust
April 1, 2015/Ganga Cosmological Parameters 17
Vibrational & Spinning Galactic Dust
April 2, 2015 Ganga/CMB & Planck 18
Polarized Foregrounds
April 1, 2015/Ganga Cosmological Parameters 19
Galactic Synchrotron & Free-Free
April 1, 2015/Ganga Cosmological Parameters 20
Galactic Carbon Monoxide & Spectra
arXiv:1303.5088v1This has been updated with the “PCCS2”
We often treat these emissions as annoyances, but many people find them
quite interesting!
April 2, 2015 Ganga/CMB & Planck 21
2013 Temperature Power Spectrum
April 2, 2015 Ganga/CMB & Planck 22
2014 Temperature Power Spectrum
April 2, 2015 Ganga/CMB & Planck 23
Power Spectra and Parameters● H0 = 67.8 ± 0.9 kms-1Mpc-1
● Ωm = 0.308 ± 0.012
● ns = 0.968 ± 0.006● τ = 0.066 ± 0.016● Neff= 3.15 ± 0.23
● Σmν < 0.23 eV
● This spectrum can be reconstructed using only six parameters – Amplitude, simple spectrum of “input” variations, baryonic & cold
dark matters, oscillation scale & optical depth (+Λ)– This simple agreement extends to polarization as well– There is no convincing evidence for extensions to the standard
model of cosmology
April 2, 2015 Ganga/CMB & Planck 24
Non-Gaussianity● We do find the ISW
bispectrum expected in a CDM Universe
● We do see non-Gaussianity from point sources
● We don't see any– Local: 0.8 ± 5.0– Equilateral: -4 ± 43– Orthogonal: -26 ± 21– (68%CL)
http://arxiv.org/abs/1502.01592
April 2, 2015 Ganga/CMB & Planck 25
Gravitational Lensing● Mass between the last
scattering surface and us lenses the CMB
● We use the deflections to infer the effective potential seen by the CMB
http://arxiv.org/abs/1502.01591
April 2, 2015 Ganga/CMB & Planck 26
Gravitational Lensing● Mass between the last
scattering surface and us lenses the CMB
● We use the deflections to infer the effective potential seen by the CMB
http://arxiv.org/abs/1502.01591
April 2, 2015 Ganga/CMB & Planck 27
Cosmic Infrared Background
● Dominates the extragalactic sky in the higher Planck frequencies
● Has a spectrum similar to Galactic dust● Tracer of star formation, much of it around z~2.● Represents material at higher redshifts than many catalogs● arXiv:1309.0382v1
April 2, 2015 Ganga/CMB & Planck 28
CIB × Lensing Potential● The CIB is the remnant of
star formation, much around z~2
● This material lenses the CMB● A cross-correlation shows
this:
● Correlations can also be done with your favorite catalog of sources, or other tracers of mass
ArXiv: 1303.5078v1
545 GHz × Φ
April 2, 2015 Ganga/CMB & Planck 29
SZ Catalog
Sunyaev-Zeldovich Effect● Hot electrons in
clusters give CMB photons “a kick”
● This allows us to detect 1653 clusters and candidates of clusters of galaxies
http://spiff.rit.edu/classes/phys443/lectures/cluster_2/sunyaev.png -- Michael Richmond
April 2, 2015 Ganga/CMB & Planck 30
Spectra Zoo
r = 0.2
Scalar TT
Tensor TT
Scalar TE
TensorTE
ScalarEE
TensorEE
Tensor BB
Lens BB
Scalar & Tensor TT, TE, EE & BB Spectra
Reionization changes the
amplitude of the anisotropies
and adds signal at the largest
angular scales
April 2, 2015 Ganga/CMB & Planck 31
Optical Depth from Large Ang. Scales
http://webcast.in2p3.fr/videos-establishing_the_planck_only_likelihood
5 10 15 20 25
70 GHz DataPlanck 2013 (τ~0.9)Planck 2015 (τ~0.7)
LFI Noise Level
April 2, 2015 Ganga/CMB & Planck 32
ReionizationLFI polarization data, together with Planck lensing and high-multipole temperature data gives a reionization optical depth, τ=0.066±0.016 and a reionization redshift of zre=8.8+1.7
-1.4. These numbers are in good agreement with those inferred from the WMAP9 polarization data cleaned for polarized dust emission using the HFI 353 GHz maps, as well as Planck temperature and lensing data (i.e., not using polarization data).
Early WMAP was here
April 2, 2015 Ganga/CMB & Planck 33
CMB: Primordial vs. Recent● The CMB has
traditionally be used to probe the early Universe– First to understand the
Universe at t > 400k years and the total energy density of the Universe
– Now to try to understand what led to our Universe (i.e., is Inflation correct, or is it something else?)
● The CMB is being used more and more as a tool to understand what is between us and the surface of last scattering– SZ effect and clusters– SZ and baryons– Lensing and Galaxy
formation– Lensing and neutrinos
April 2, 2015 Ganga/CMB & Planck 34
Relic Gravitational Waves – B-Modes
http://bicepkeck.org/visuals.html
April 2, 2015 Ganga/CMB & Planck 35
Polarization of the CMB
April 2, 2015 Ganga/CMB & Planck 36
Spectra Zoo & B-Modes
r = 0.2
Scalar TT
Tensor TT
Scalar TE
TensorTE
ScalarEE
TensorEE
Tensor BB
Lens BB
Dorothea Samtleben will discuss this as well
'r' quantifies
the fraction of power in
tensors versus scalars
April 2, 2015 Ganga/CMB & Planck 37
Inflation● ns = 0.968 ± 0.006● Tensor-to-scalar ratio: r < 0.11 (95% C.L.)● Further measurements of B-mode polarization will
improve limits on “r”
arXiv:1502.02114n
s →
r
April 2, 2015 Ganga/CMB & Planck 38
BICEP Sees r ~ 0.2
● “The observed B-mode power spectrum is well-fit by a lensed-LCDM + tensor theoretical model with tensor/scalar ratio r=0.20+0.07
-
0.05.” -- BICEP2 I: Detection of B-mode Polarization at Degree Angular Scales (2014)
● We were looking for a needle in a haystack, but instead we found a crowbar. -- Clem Pryke
● “... the fractional contribution of tensor modes is limited to r < 0.13 (95% CL)” -- Nine-year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Cosmological Parameter Results (2012)
● “Planck establishes an upper bound on the tensor-to-scalar ratio of r < 0.11 (95% CL).” -- Planck 2013 results. XXII. Constraints on inflation.
April 2, 2015 Ganga/CMB & Planck 39
April 2, 2015 Ganga/CMB & Planck 40
Spectral Subtraction Analysis● We also try a simple
analysis, subtracting the scaled 150x353 spectrum from the 150x150 spectrum– This approximates a map-
based cleaning● The resulting r constraint is
similar (although a little less powerful than that from the “full” analysis)
● r<0.12 from BICEP+Planckhttp://adsabs.harvard.edu/abs/2015arXiv150202114P
April 2, 2015 Ganga/CMB & Planck 41
Fig. 8: Best Parts of the Polarized Sky● Value of BB spectrum at ℓ=80, normalized to a spectrum with r=1. – Deep red is r~10– Orange/red is r~1– Blue/cyan is r~0.1– Deep blue is r~0.01
● Computed from the 353 GHz data and extrapo-lated to 150 GHz using power law above
Signal
Uncertainty
April 2, 2015 Ganga/CMB & Planck 42
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April 2, 2015 Ganga/CMB & Planck 43
Planck Release Schedules● What has been released:
–
–
● High-ℓ Likelihood: CMB+Lensing, Temperature+Polarization – Low-l: Based on LFI 70 GHz (replacing WMAP)
● Lensing● SZ, point sources, ...● Galactic Emissions● ...
April 2, 2015 Ganga/CMB & Planck 44
Acknowledgements