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Observational Cosmology Lab University of Wisconsin-Madison

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Presentation on theme: "Observational Cosmology Lab University of Wisconsin-Madison"— Presentation transcript:

1 Observational Cosmology Lab University of Wisconsin-Madison
Cosmic Microwave Background polarization observations with the POLAR and COMPASS experiments Christopher O’Dell Observational Cosmology Lab University of Wisconsin-Madison

2 TALK OUTLINE CMB Introduction CMB Polarization Description/Motivation POLAR: Experiment/Analysis/Results COMPASS and Future Prospects

3 Cosmic Microwave Background: 3 Characteristics
2. Spatial Anisotropy T = K Tcmb = K +/ mK 1. Spectrum T ~ 20 K

4 Cosmological Theories Anisotropy Data in 2001
Church, Jaffe, & Knox 2001 astro-ph/

5 Cosmological Parameters in 2001

6 3rd CMB Characteristic: Polarization
At last scattering, a quadrupole in temperature anisotropy generates a polarized CMB signal.

7 Rotation of Coordinates by angle a
POLARIZATION MATH Stokes’ Parameters Intensity Linear Polarization Circular Polarization Rotation of Coordinates by angle a

8 The E-B Decomposition Gradient-Type (E) : Symmetric Under Rotation
Symmetric Under Parity Curl-Type (B): Symmetric Under Rotation Anti-symmetric Under Parity Power Spectra: TT : Anisotropy EE : E-type Polarization BB : B-type Polarization TE : Temp-Epol Cross Correlation Zaldarriaga & Seljak, 1998

9 Hu & Dodelson (Annual Reviews 2002)
The Four CMB Power Spectra TT TE Hu & Dodelson (Annual Reviews 2002)

10 Why Measure CMB Polarization??
Is a fundamental prediction of the standard cosmological model. Helps break degeneracies in determining fundamental cosmological parameters. Probes Reionization History of the Universe. B-modes are directly sensitive to primordial gravitational waves; the amplitude of the BB spectrum is proportional to the square root of the energy scale of inflation. They also help characterize the tensor-to-scalar ratio, r. Polarization is required to truly test adiabaticity of the primordial seeds of structure. Parameter estimation is seriously degraded when a mixture of initial fluctuation types is allowed. We often see something new and unexpected with each new window on the universe!

11 No Reionization. Prms ~ 0.5 K Zaldarriaga, 2001

12 Reionization at z ~ 30 Prms ~ 3.2 K t = 0.3 , Zre ~ 30
Zaldarriaga, 2001

13 1965 1979 1983 1995 Zre ~ 30 Reionization Peak Josh Gundersen, 2001

14 Polarization Observations of Large Angular Regions (POLAR)
A. de Oliveira-Costa (UPenn) J. Gundersen (Miami) B. Keating (Caltech) S. Klawikowski (UW-Madison) C. O’Dell (UW-Madison) L. Piccirillo (Cardiff) N. Stebor (UW-Madison) D. Swetz (UW-Madison) M. Tegmark (UPenn) P. Timbie (UW-Madison)

15 The Spinning Correlation Polarimeter
x y CMB Ground Screens Ex Ey OMT Gx Gy 0°, 180° Phase Shifter Multiplier

16 POLAR Main Features Clean, simple design: no lenses or mirrors no magnetic or moving parts (excepting overall rotation) Corrugated conical feed horn achieves 7° beam with very low sidelobes. HEMT amplifiers (25 K noise temperature, NET ~ 800 K • sec-1/2) Commercial Cryocooler (no liquid cryogens). Frequency bands: GHz, 3 sub-bands (plus basic sensitivity to Ix and Iy ).

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20 Outer Ground Shield Clam-Shell Dome Clam-Shell Dome Inner Ground Shield 20 K Dewar

21 Q and U at ~ 20 pixels on the sky, on a 7° ring at declination 43°
POLAR Scan Strategy Q and U at ~ 20 pixels on the sky, on a 7° ring at declination 43°

22 Atmospheric Emission at Sea Level
H2O O2 Broad Line Emission Unpolarized in absence of external fields Possible O2 Zeeman splitting by earth’s B-field Negligible Will add to system noise, and affect required integration time.

23 Stability and Sensitivity

24 Polarized Foregrounds Power Spectra
(30%) (3%) Josh Gundersen, 1999

25 from Pine Bluff, Wisconsin
Observations and Data Selection March 1st – May 31st, 2000 from Pine Bluff, Wisconsin

26 Mapmaking Data Vector True Sky Map Noise Vector Pointing Matrix
Problem : Re-construct the map from your data that is closest to the true, underlying map. Solution : “Minimum Variance Mapmaking” (not simply weighted averaging in the presence of 1/f noise)

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28 Multi-Frequency Maps

29 Flat Band-Power Model :
E, B Spectra have constant power at all scales, characterized by variances : (TE2 , TB2) Full 2D Likelihood: Prior Constraint that TB = 0

30 Modern Polarization Upper Limits and POLAR band-powers
0.1 105 Modern Polarization Upper Limits and POLAR band-powers 104 103 E-Mode Limits B-Mode Limits 100 PIQUE CBI ATCA 10 POLAR 1.0 0.1 10 100 1000

31 Onward! -> COMPASS UW-Madison UCSB Cardiff
UC-Davis Caltech Rome III U-Miami

32 CMB Polarization: Full Speed Ahead!
Experiment Date Total Sensitivity l-range DASI (HEMTs) Full Year ~ 1 uK MAXIPOL (Spiderwebs) Mid May ~ 2 uK B2.002K (PSBs) December < 1 uK CBI (HEMTs) Full Year ~ 1 uK ? MAP (HEMTs) Ongoing (data ~ 1yr?) ??? QUEST, BICEP, SPORT, ROPE, CAPMAP, etc. ??? PLANCK (HEMT/PSB) 2007? < 0.1 uK


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