QUaD: A CMB Polarization Experiment … First Year Results, arXiv:0705.2359v1 Robert B. Friedman The University of Chicago GLCW8 - 5.31.07.

Slides:



Advertisements
Similar presentations
The second LDB flight of BOOMERanG was devoted to CMB polarization measurements Was motivated by the desire to measure polarization : –at 145 GHz (higher.
Advertisements

A Crash Course in Radio Astronomy and Interferometry: 4
QUIET Q/U Imaging ExperimenT Osamu Tajima (KEK) QUIET collaboration 1.
First results from QUIET Osamu Tajima (KEK) The QUIET Collaboration 1.
The Ability of Planck to Measure Unresolved Sources Bruce Partridge Haverford College For the Planck Consortium.
Clouds and the Earth’s Radiant Energy System NASA Langley Research Center / Atmospheric Sciences Methodology to compare GERB- CERES filtered radiances.
The Sunyaev-Zel’dovich Effect Jason Glenn APS Historical Perspective Physics of the SZ Effect Previous Observations.
Systematic effects in cosmic microwave background polarization and power spectrum estimation SKA 2010 Postgraduate Bursary Conference, Stellenbosch Institute.
Photo: Keith Vanderlinde Detection of tensor B-mode polarization : Why would we need any more data?
SIW 2003 The antenna element Ravi ATNF, Narrabri 1.The role of the antenna in a Fourier synthesis radio telescope 2.The Compact array antenna.
29 June 2006Bernard's Cosmic Stories1 1 st results from the QUaD CMB polarisation experiment Michael Brown (University of Edinburgh)
K. Ganga – CMB Science and Observations 1 Rencontres du Vietnam /08 The QuaD CMB Polarization Experiment K. Ganga APC.
Component Separation of Polarized Data Application to PLANCK Jonathan Aumont J-F. Macías-Pérez, M. Tristram, D. Santos
Cosmology After WMAP David Spergel Cambridge December 17, 2007.
K.S. Dawson, W.L. Holzapfel, E.D. Reese University of California at Berkeley, Berkeley, CA J.E. Carlstrom, S.J. LaRoque, D. Nagai University of Chicago,
N. Ponthieu Polarization workshop, IAS, Orsay, 09/15/ N. Ponthieu (IAS) The conquest of sky polarization The upper limits era First detections Prospects.
BICEP: B ackground I maging of C osmic E xtragalactic P olarization “The Muscle Behind Curls” Jamie Bock Hien Nguyen Caltech/JPL Andrew Lange Brian Keating.
CMB polarisation results from QUIET
Advanced Cosmology Bolometer Array Receiver (ACBAR) on Viper Jeff Peterson - CMU –Ravinder Bhatia (Caltech) –Jamie Bock (JPL) –Andrew Lange (Caltech) –Peter.
CMB Polariztion B. Winstein Chicago, CfCP General Introduction to the Problem The CAPMAP Solution.
(Rajib Saha,Pankaj Jain,Tarun Souradeep, astro-ph/ ) A Blind Estimation of Angular Power Spectrum of CMB Anisotropy from WMAP.
Einstein Polarization Interferometer for Cosmology (EPIC) Peter Timbie University of Wisconsin - Madison Beyond Einstein SLAC May
Ground-based and Future Observations of the Cosmic Microwave Background Anthony Lasenby Astrophysics Group, Cavendish Laboratory, Cambridge University.
1 CMB Polarimetry with BICEP: Probing Inflationary Gravitational Waves IAS - Polarization 2005 Denis Barkats.
Separating Cosmological B-Modes with FastICA Stivoli F. Baccigalupi C. Maino D. Stompor R. Orsay – 15/09/2005.
Title Here Probing the Epoch of Reionization with the Tomographic Ionized-carbon Mapping Experiment (TIME) Jamie Bock Caltech / JPL CCAT Workshop, Boulder.
P olarized R adiation I maging and S pectroscopy M ission Probing cosmic structures and radiation with the ultimate polarimetric spectro-imaging of the.
The Implication of BICEP2 : Alternative Interpretations on its results Seokcheon Lee SNU Seminar Apr. 10 th
The “QUEST” for CMB Polarization Walter K. Gear Cardiff University.
Science Impact of Sensor Effects or How well do we need to understand our CCDs? Tony Tyson.
Astronomy & Astrophysics Advisory Committee (AAAC) May 11, 2006 Vladimir Papitashvili Antarctic Sciences Section Office of Polar Programs National Science.
US Planck Data Analysis Review 1 Peter MeinholdUS Planck Data Analysis Review 9–10 May 2006 Where we need to be 2 months before launch- Instrument view.
Update on QUaD Sarah Church QUaD Collaboration Funded: National Science Foundation Astronomy Program and Office of Polar Programs.
Beijing, Feb 3 rd, % e+ Poalarization 1 Physics with an initial positron polarisation of ≈30% Sabine Riemann (DESY)
QUIET Q/U Imaging ExperimenT. QUIET Project Miami Physics Conference 2009 December 16 Raul Monsalve for the QUIET Collaboration University of Miami QUIET.
US Planck Data Analysis Review 1 Christopher CantalupoUS Planck Data Analysis Review 9–10 May 2006 CTP Working Group Presented by Christopher Cantalupo.
Cosmic Microwave Background Carlo Baccigalupi, SISSA CMB lectures at TRR33, see the complete program at darkuniverse.uni-hd.de/view/Main/WinterSchoolLecture5.
The Einstein Inflation Probe: Experimental Probe of Inflationary Cosmology (EPIC) Study Jamie Bock Jet Propulsion Laboratory / Caltech Charles BeichmanRobert.
Joint analysis of Archeops and WMAP observations of the CMB G. Patanchon (University of British Columbia) for the Archeops collaboration.
Cosmic Microwave Background Carlo Baccigalupi, SISSA CMB lectures at TRR33, see the complete program at darkuniverse.uni-hd.de/view/Main/WinterSchoolLecture5.
The Millimeter-wave Bolometric Interferometer (MBI) Peter Hyland University of Wisconsin – Madison For the MBI Collaboration New Views Symposium December.
B Polarization Measurement of the CMB
Kalanand Mishra April 27, Branching Ratio Measurements of Decays D 0  π - π + π 0, D 0  K - K + π 0 Relative to D 0  K - π + π 0 Giampiero Mancinelli,
Sept. 18, 2008SLUO 2008 Annual Meeting CMB Polarization Measurements Sarah Church John Fox, Chao-Lin Kuo, Sami Tantawi, Dan Van Winkle KIPAC/Stanford Physics/SLAC.
QUIET Experiment Rencontres de Moriond 2010 March 14 th, 2010 Akito KUSAKA (for QUIET collaboration) University of Chicago, EFI and KICP.
A New Bound on the Radar Cross-section of the Sun Bill Coles, UCSD Mike Sulzer and John Harmon, NAIC Jorge Chau and Ron Woodman, JRO We have not observed.
Intrinsic Short Term Variability in W3-OH and W49N Hydroxyl Masers W.M. Goss National Radio Astronomy Observatory Socorro, New Mexico, USA A.A. Deshpande,
The Very Small Array Angela Taylor & Anze Slosar Cavendish Astrophysics University of Cambridge.
Chao-Lin Kuo Stanford Physics/SLAC
High Resolution Measurements of CMB Anisotropies with ACBAR U.C. Berkeley: W.L. Holzapfel (co-PI) M.D. Daub M. Lueker Case-Western: J. Ruhl (co-PI) J.
Observing Strategies at cm wavelengths Making good decisions Jessica Chapman Synthesis Workshop May 2003.
EBEx foregrounds and band optimization Carlo Baccigalupi, Radek Stompor.
Experimental Cosmology Group Oxford Astrophysics Overview CLOVER is a UK-led experiment to detect the B-mode polarisation of the Cosmic Microwave Background.
The Planck Satellite Hannu Kurki-Suonio University of Helsinki Finnish-Japanese Workshop on Particle Cosmology, Helsinki
The Australia Telescope National Facility Ray Norris CSIRO ATNF.
Planck Report on the status of the mission Carlo Baccigalupi, SISSA.
Fast or slow positron spin flipping Sabine Riemann (DESY) November 17, 2008 ILC08, University of Illinois - Chicago.
MONALISA: The precision of absolute distance interferometry measurements Matthew Warden, Paul Coe, David Urner, Armin Reichold Photon 08, Edinburgh.
Blind Component Separation for Polarized Obseravations of the CMB Jonathan Aumont, Juan-Francisco Macias-Perez Rencontres de Moriond 2006 La.
150GHz 100GHz 220GHz Galactic Latitude (Deg) A Millimeter Wave Galactic Plane Survey with the BICEP Polarimeter Evan Bierman (U.C. San Diego) and C. Darren.
2-year Total Intensity Observations year Polarization Observations Cosmic Background Imager Tony Readhead Zeldovich celebration.
CMB polarization observations with the POLAR and COMPASS experiments Christopher O’Dell Observational Cosmology Lab University of Wisconsin-Madison
Kalanand Mishra February 23, Branching Ratio Measurements of Decays D 0  π - π + π 0, D 0  K - K + π 0 Relative to D 0  K - π + π 0 decay Giampiero.
BICEP2 Results & Its Implication on inflation models and Cosmology Seokcheon Lee 48 th Workshop on Gravitation & NR May. 16 th
Detecting the CMB Polarization Ziang Yan. How do we know about the universe by studying CMB?
Observational Cosmology Lab University of Wisconsin-Madison
Observing and Data Reduction
12th Marcel Grossman Meeting,
A Measurement of CMB Polarization with QUaD
Molecular Imager: Focal Plane Array
Presentation transcript:

QUaD: A CMB Polarization Experiment … First Year Results, arXiv: v1 Robert B. Friedman The University of Chicago GLCW

What I Will Attempt to Cover  CMB Pol.  What is QUaD?  Analysis Techniques.  First Year Results ( arXiv: v1) & Future GLCW

CMB Polarization Science  Curves are WMAP3  EE Polarization alone cannot compete with TT for parameters (save for  )  It’s a paradigm check  BB is the hot stuff!!!  Likely below the reach of current experiments (QUaD)  Probes inflation & foregrounds through lensing QUaD will nail these GLCW

Who is QUaD?  Chicago  Clem Pryke, Tom Culverhouse, myself, John Carlstrom, Erik Leitch (JPL), Robert Schwartz (SP)  Caltech  John Kovac, Ken Ganga (Paris), Andre Lange, Jamie Bock  Stanford  Sarah Church, Ed Wu, Jamie Hendricks, Ben Rusholme, Melanie Bowden, Keith Thompson  Cardiff  Walter Gear, Mike Zemcov, Nutan Rajguru, Angiola Orland, Peter Ade, Simon Melhuish, Lucio Piccirillo  Edinburgh  Andy Taylor, Michael Brown, Patricia Castro (Lisbon)  Maynooth  Anthony Murphy, Creidhe O’Sullivan, Gary Cahill GLCW

What is QUaD?  QUaD stands for QUEST at DASI  QUEST is the bolometer array receiver  DASI interferometer first detected polariztion  High Resolution  sensitive to modes up to l ~2500  Receiver focal plane consists of 31 Polarization Sensitive Bolometer pairs  19 at 150GHz and 12 at 100GHz.  2.6m Cassegrain focus assembly mounted on the DASI platform  tri-axial orientation; AZ, EL, DK  foam cone secondary support GLCW

The Foam Cone  Typical radio telescopes use metallic secondary support legs  Can induce spurious polarization  Foam Cone made from mm-wave transparent Zotefoam.  Axially symmetric rigid cone structure adds stability ME GLCW

Map Making  Time Ordered Data (TOD) is “field differenced” first  Cancels common ground signal  3rd order polynomial removed from raw TOD  Cuts down “1/f noise” (mostly atmosphere ie. large scale variations like clouds).  PSB pair TOD summed and differenced  Sum produces Intensity or T signal  Difference used for stokes Q & U  Inverse variance weighting applied to summations  Variance map simultaneously constructed GLCW

QUaD E and B Maps  Top Row: E & B Polarization Signal  No BB signal expected!  Bottom Row: “Deck” Jackknife … should look like noise. GLCW

Spectra Estimation Procedure  Generate random CMB realizations, observe with simulated telescope  Signal only, noise only and signal plus noise sim TOD for sum/diff  Include all known parameters and uncertainties (ie. beam shapes, polarization efficiencies, etc.)  Construct maps from sim TOD and calculate sim spectra from them  Use sims to correct observed power spectra and estimate error bars  Subtract noise power measured from noise only sim spectra  Estimate filter/beam suppression measured as the ratio of signal only sim spectra vs. input spectra  variance per band in signal plus noise spectra is the ~error GLCW

Jackknife Spectra  Jackknife tests  Difference maps from independent data sets  Frequency, Deck Angle, Scan Direction, Focal Plane and Season Should be consistent w/ ZERO! GLCW

The Future of QUaD  Preliminary 1st Season Analysis Represents 67 of ~200 days already in the can.  See results arXiv: v1  3rd Season observations currently underway.  Will likely provide at least another ~70 more days  Coming Soon…  Reduced errorbars (more time)  New and improved beam models  Better control of systematics GLCW