k. ganga – cmb science and observations 1 rencontres du vietnam - 2006/08/09 cmb science and...
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K. Ganga – CMB Science and Observations 1 Rencontres du Vietnam - 2006/08/09
CMB Science and
Observations
K. Ganga
K. Ganga – CMB Science and Observations 2 Rencontres du Vietnam - 2006/08/09
The CMB● The CMB is a blackbody
at T = 2.73 K.
● The most prominent “anisotropy” in the CMB, with amplitude of about 0.1%, is due to our motion with respect to the CMB rest frame.
● Further anisotropies are at the level of 0.001% and lower (or much lower)
K. Ganga – CMB Science and Observations 3 Rencontres du Vietnam - 2006/08/09
Observerz =1000 z = infinity
Plasma
Recombination
T=2.73K
Plasma
Horizon ~1o
z =1000
Plasma
Recombination
Gravitational lensing
T=2.73K
Reionisation
Observer
The CMB again...Thanks to A. Taylor
K. Ganga – CMB Science and Observations 4 Rencontres du Vietnam - 2006/08/09
T on super-horizon scales (>1o)• Sachs-Wolfe Effect: Gravitational redshift due to
photons climbing out of potential wells,
T13
A. Taylor
K. Ganga – CMB Science and Observations 5 Rencontres du Vietnam - 2006/08/09
Acoustic Oscillations
K. Ganga – CMB Science and Observations 6 Rencontres du Vietnam - 2006/08/09
Measuring Curvature
Flat
Closed
Open
1
2
3
Acoustichorizon
(same for all)
vs tdec
J. Ruhl
B. Crill
K. Ganga – CMB Science and Observations 7 Rencontres du Vietnam - 2006/08/09
Baryons change the “effective mass”
W. Hu
K. Ganga – CMB Science and Observations 8 Rencontres du Vietnam - 2006/08/09
How Parameters are Fit
Parameters are found by making spectra for the
range of models of interestand finding which has the “best” chi-squared giventhe actual data and some
“prior” information.
Angular spectrum varies mostly with
bcdmH0,ns
K. Ganga – CMB Science and Observations 9 Rencontres du Vietnam - 2006/08/09
'Degeneracies' require other data
lpeak200 0-1/2
Simulated “Pretty flat” models
tot = 1
K. Ganga – CMB Science and Observations 10 Rencontres du Vietnam - 2006/08/09
A little help from our friends...
From: Lewis & Bridle 2002
Red: Pre-WMAP CMB data
Blue: CMB data w/ HST
Yellow: CMB data w/ HST, 2dF, BBN
K. Ganga – CMB Science and Observations 11 Rencontres du Vietnam - 2006/08/09
The CMB Temperature Power Spectrum
Archeops/ARGO/ATCA/BAM/DASI/DMR/FIRS/IAB/MAX(IMA)/OVRO/Python/QMAP/Relict/Saskatoon/South Pole/Tenerife/Toco/Viper/White Dish/...
WMAP/Acbar/BOOMERanG/CBI/VSA
K. Ganga – CMB Science and Observations 12 Rencontres du Vietnam - 2006/08/09
Quadrupole Scattering
e-
CMB polarization is caused by Thomson scattering of a local
quadrupole (Rees, 1968).
The polarized component of the
CMB must be small, as it
results from local temperature anisotropies.
K. Ganga – CMB Science and Observations 13 Rencontres du Vietnam - 2006/08/09
Polarization has been measured
Lens
IGW
DASI, CBI, BOOMERanG and CAPMAPhave all published polarization detections.
DASI
WMAP
K. Ganga – CMB Science and Observations 14 Rencontres du Vietnam - 2006/08/09
Parameters
K. Ganga – CMB Science and Observations 15 Rencontres du Vietnam - 2006/08/09
Can decompose Q & U into:E-modes (even-parity):
(or grad)
B-modes (odd-parity): (or curl)
E-modes produced by all quadrupole sources (velocity gradients and gravitational waves)
B-modes produced by gravitational waves and lensing of E-modes
The E/B Decomposition
Pure E Pure B
Wayne Hu
K. Ganga – CMB Science and Observations 16 Rencontres du Vietnam - 2006/08/09
Lensing transform E to B
● Converts E-modes to B-modes– Confusion limit to measuring the gravitational wave
component– Interesting signal in itself, probing growth of structure
from present-day to epoch of decoupling
K. Ganga – CMB Science and Observations 17 Rencontres du Vietnam - 2006/08/09
Inflation Constraints
V
Einflation
~ mpl×r¼
mpl2
2V 'V
2
1 ;
mpl2 V ' 'V
1 ;
r 12.4 ;
n 1 6 2 ;
Liddle & Lyth, 2000
K. Ganga – CMB Science and Observations 18 Rencontres du Vietnam - 2006/08/09
Predicted SpectraTT
EE
Lens
T/S=0.005
T/S=0.05
T/S=0.0005
BB
IGW
K. Ganga – CMB Science and Observations 19 Rencontres du Vietnam - 2006/08/09
Future Observations
Lawrence, C.R., Proceedings of Science (CMB2006)
K. Ganga – CMB Science and Observations 20 Rencontres du Vietnam - 2006/08/09
Sensitivity to Q or U (K s1/2)
780
250
170
HFI spec
3716225353
265825217
234127143
CMB BLIPCMB + Inst. BLIP
No of feeds per Q (or U)
Beam (arcmin)
Frequency
(GHz)
The Planck HFI
• 50 feeds in a focal plane of ~ 1kg at 100mK• Focal plane area ~ 2 square degrees• Instantaneous sky coverage per polarization-
sensitive frequency about: 0.1 square degrees
The HFI also has channels at 100, 545 and 850 GHz that are not polarization sensitive
K. Ganga – CMB Science and Observations 21 Rencontres du Vietnam - 2006/08/09
Predicted Planck Measurements
r=0.1,τ=0.17
K. Ganga – CMB Science and Observations 22 Rencontres du Vietnam - 2006/08/09
How to go deeper● Planck can detect r~0.1● Planck is ~2 times BLIP● Planck has ~10
detectors covering ~0.1 degree2 per frequency
● Planck observes ~1 yr.● In the BLIP limit,
ignoring cosmic variance, Δr~ σ2 ~(N
detectors•Time)-1
● A future mission should:– Achieve BLIP– Observe longer (~2)
● ~2 for satellites● John will discuss ground-
based– Use many more pixels
● To go much deeper, we must use arrays.
K. Ganga – CMB Science and Observations 23 Rencontres du Vietnam - 2006/08/09
Example: EPIC
J. Bock
K. Ganga – CMB Science and Observations 24 Rencontres du Vietnam - 2006/08/09
WMAP Foregrounds
74.3% of sky
K. Ganga – CMB Science and Observations 25 Rencontres du Vietnam - 2006/08/09
BOOMERanG and CBI Measurements
Montroy, et al.
Neither BOOMERanG nor CBIhave detected any BB at the levelof the EE polarization signals.This limits the foregrounds in theirregions.
K. Ganga – CMB Science and Observations 26 Rencontres du Vietnam - 2006/08/09
Fin
K. Ganga – CMB Science and Observations 27 Rencontres du Vietnam - 2006/08/09
Symmetry?
K. Ganga – CMB Science and Observations 28 Rencontres du Vietnam - 2006/08/09
WMAP: w versus k
K. Ganga – CMB Science and Observations 29 Rencontres du Vietnam - 2006/08/09
WMAP: w versus m