No Slide Title

Total Page:16

File Type:pdf, Size:1020Kb

No Slide Title Program for Small Scale Anisotropy Measurements and the Ability to set Limits on Inflation. A. Lee, L.Page and J. Ruhl 1 l>1000 CMB/SZ Experiments ACBAR (Bolometric feed array) ACT SPT AMiBA (Taiwan, Interferometer) SuZie Upgrade AMI (UK, Interferometer) SZA (Interferometer) APEX VSA (Interferometer) Bolocam (Bolometric Camera, CSO) CBI (Interferometer) 2 Selected Bolometer-Array and SZ Roadmap APEX SCUBA2 (~400 bolometers) (12000 bolometers) SZA Chile (Interferometer) Owens Valley ACT (3000 bolometers) Chile CMBPOL 2003 2005 2007 2004 2006 2008 SPT ALMA Polarbear-I (1000 bolometers) (Interferometer) (300 bolometers) South Pole Chile California Planck (50 bolometers) L2 3 ACT Collaboration Cardiff NASA/GSFC Princeton Peter Ade Domonic Benford Joe Fowler Cindy Hunt Jay Chervenak Norm Jarosik Phil Mauskopf Harvey Moseley Robert Lupton Carl Stahle Bob Margolis Columbia Ed Wollack Lyman Page Uros Seljak Amber Miller Penn David Spergel CUNY Angelica de Oliveira Costa Suzanne Staggs Martin Spergel Mark Devlin Simon Dicker Rutgers Haverford Bhuvnesh Jain Laura Ferrarese Steve Boughn Raul Jimenez Arthur Kosowsky Bruce Partridge Jeff Klein Jack Hughes Max Tegmark Ted Williams INOAE Licia Verde David Hughes Univ. de Catolica UMass Hernan Quintana NIST/Boulder Grant Wilson Univ. of Toronto Randy Doriese Univ. of British Columbia Kent Irwin Barth Netterfield Mark Halpern 4 Science: Observations: AtacamaACT Cosmology Telescope Growth of structure CMB: l>1000 Eqn. of state Cluster (SZ, KSZ X-rays, & optical) Neutrino mass Diffuse SZ Ionization history OV Power spectrum Lensing X-ray Optical Theory 5 Goals: Cosmological Parameters CMB Cosmic Structure Optical Coordinated ν Mass Approach +/- 0.1eV X-Ray Equation of State – w +/- 0.1 Theory Signature of Galactic First Stars Studies 6 Cosmic Timeline • First galaxies • Universe is reionized • Cluster formation: Sunyaev-Zel’dovich (SZ) • Ostriker-Vishniac • Kinematic SZ • Diffuse thermal SZ • Lensing of the CMB • Extraction of • The growth of structure is sensitive to w and mn cosmological parameters • Rich additional science from correlations among effects • Initial conditions for structure formation z = 1100 z = 6-7 z = 1 z = .25 now Primary CMB OV Diffuse Thermal SZ CMB Lensing Cluster Surveys 7 Inflation At low l<100, a clear signature would be the detection of B-modes or unambiguous measure of r based on TT, TE, EE + galaxies. Unadulterated (circa 1988) inflation gives: r=0.27. This implies a BB signal of roughly 0.01 uK2 at l=5. Current limit r<0.36 [95%] (Seljak et al. 2004) based on TT and TE. ns=0.95 +/- 0.02. The current limit is 0.98+/-0.02 (Seljak et al. 2004) [WMAP alone 0.99+/-0.04] dns/dlnk = 0. The current limit is -0.003+/- 0.01. (Seljak et al. 2004) 8 Lay of the Low l Land Current limit G-waves on tensors decay once inside the B modes from horizon. tensors only. B modes from lensing of E modes. Reionization peak Horizon size at decoupling (zdec=1089) (zr=20) 9 What does l>1000 add? The limits on ns and dns/dlnk come from the combination of WMAP and SDSS + Lya. These latter two probe high l (or high k). High l CMB measurements allow us to get at these parameters with the CMB alone, which should be less susceptible to “astrophysical systematics” than other measurements. Two mechanisms: Larger lever arm for measuring the slope. Breaking the ns-tau-r degeneracy. High l CMB experiments, when combined with WMAP, can reach 1% accuracy on ns but needs <1% calibration.. 10 Simulations of mm-wave data. <1% 1.40 Survey area ≈ 2% High quality area 150 GHz SZ Simulation MBAC on ACT PLANCK Burwell/Seljak 1.7’ beam MAP ACT PLANCK Target Sensitivity de Oliveira-Costa Hot electron gas ACT Bands imposes a unique spectral signature 145 GHz decrement 220 GHz null 270 GHz increment 1.4°x 1.4° NO SZ Contribution in Central Band 12 145 GHz Maps Map Components Components Summed to Scale CMB SZ 1.4°x 1.4° KSZ/OV Point Sources 13 220 GHz Maps Map Components Components Summed to Scale CMB SZ 1.4°x 1.4° KSZ/OV Point Sources 14 270 GHz Maps Map Components Components Summed to Scale CMB SZ 1.4°x 1.4° KSZ/OV Point Sources 15 Existing PUDs 3.2 mm SHARC II Need picture PI D. Dowell PUD Architecture. Semiconductors Completed “close-packed” 12x32 bolometer array Dowell et al, 2003 SHARC II 12x32 Popup Array FIBRE Torsional yoke attachment PI D. Benford PUD Architecture. TES+SQUID Mux 1 mm Coming soon: SCUBA SCUBA-2 PD W. Duncan HAWC Linear array after folding PI A. Harper One element of array 16 Where? The Atacama in Chile: The ideal site for our science. • 5200 meter elevation • One of driest places on planet • The future site for ALMA • Logistical support available • Only 26 hours travel from East Coast to site 17 Cross Linked Scan Strategy is Crucial to Making Maps on Degree Angular Scales • 240 square degrees in circle • 100 square degrees for CMB • Rich Galactic data set QuickTime™ and a BMP decompressor are needed to see this picture. 18 Cross-linked and Overlapping Scans • Subtract a single level and gradient from East and West scans to link at the center. • The largest total offset before full interlocking mapping solution, at l ~ 300, is less than 100 µK. East Scan West Scan • Each detector samples all points of the map without EVER changing elevation. • Multiple pixels per PSF. All scans done at constant elevation. • Produce many 1.4° x 1.4° maps. Cross-linking key to WMAP, PLANCK, BOOMERanG, MAXIMA, QMAP 19 Timeline 20 10m South Pole Telescope (SPT) and 1000 element Bolometer Array Low noise, precision telescope SZE and CMB Anisotropy • 20 um rms surface - 4000 sq deg SZE survey • 1 arc second pointing - deep CMB anisotropy fields • 1.0 arcminute at 2 mm - deep CMB Polarization fields • ‘chop’ entire telescope • 3 levels of shielding - ~1 m radius on primary People - inner moving shields Carlstrom (UC) - outer fixed shields Holzapfel (UCB) Lee (UCB,LBNL) Leitch (UC) Meyer (UC) Mohr (UIUC) Padin (UC) 1000 Element Bolometer Array Pryke (UC) - 3 to 4 interchangeable bands Ruhl (UCSB) (90) 150, 250 & 270 GHz Spieler (LBNL) - APEX-SZ style horn fed spider web absorbers Stark (CfA) NSF-OPP funded & scheduled for Nov 2006 deployment DoE (LBNL) funding of readout development 21 SPT Science Goals • Galaxy Cluster Surveys » High-ell primary and kSZ/OV • Polarization 22 Science Goal #2: Secondary CMB 1. Measure the SZ power spectrum after removing obvious clusters… 2. Measure CMB-spectrum power spectrum at high l after removing thermal SZ signal… requires multiple colors. 500 sq. deg. surveys, Noise is on CMB-only after perfect tSZ subtraction. Figure: T. Crawford, spectra from W. Hu 23 Telescope Design Goals 1. Angular resolution for clusters (~ 1') at 150 GHz: Originally 8m + (1m radius “guard ring”), now 10m precision surface, no “guard ring” 2. Observe CMB & foregrounds from 1-3mm rms < 1mm/100 = 10 microns on small scales, rms < 1mm/20 = 50 microns on large scales pointing reconstruction ~ 1 arcsecond rms 3. Surveys ⇒ 1° diameter field of view at 150 GHz 4. Low offsets, low loading, low sidelobes fixed Gregorian w/ cold secondary and stop, 2 levels of ground shields. 5. Capable of sub-mm observations in the future rms < 20 microns overall (in future) 6. Flexibility for future use pure parabolic primary, large optics cabin 24 The Facility and Site Moon Door Existing Dark Sector Laboratory 25 Optical Design: Off-axis Gregorian Parabolic Primary focal plane (f/0.7) Elliptical lens Secondary Note: no chopper. S. Padin 26 10 Kelvin Secondary and Baffle 4 K plastic 300mK 300mK 10 K 10 K black 27 Telescope Drive components Receiver cabin are all in docks to control warm room for access environment 28 Structure and Shielding 144’ across Occultation limit: 28° Inner Shield (moves) 47’ high Outer Shield (fixed) To DSL 29 SZ Focal Plane 2fλ Feedhorn Coupled, ~1000 elements Horn array plate Bolometers Figure: W. Holzapfel 30 TES Bolometer Array 1 real wedge, 5 “Photoshop” SiN suspended web Cryogenics: Cooled with closed cycle 3He and pulse tubes, no LHe supply… Adrian Lee, UC Berkeley, APEX prototype 31 Band selection: which of 90, 150, 220, 270, 345 GHz ? CMB 150 + 220 GHz Thermal SZ IR point sources 270 GHz Radio point sources 90 GHz ? (but resolution gets worse…) Expected performance of these bands if used on the SPT (trans) 32 Ongoing Work Band selection: need more info on radio point sources populations, their correlations with clusters. Currently doing simulations to optimize bands and weighting… Depth vs. Area: more simulations… Scan speeds and patterns: more simulations with model atmosphere, elevation scanning, etc… + hardware, hardware, hardware… Planned First Observing Season: Austral Winter 2007 33 END 34.
Recommended publications
  • CMB Telescopes and Optical Systems to Appear In: Planets, Stars and Stellar Systems (PSSS) Volume 1: Telescopes and Instrumentation
    CMB Telescopes and Optical Systems To appear in: Planets, Stars and Stellar Systems (PSSS) Volume 1: Telescopes and Instrumentation Shaul Hanany ([email protected]) University of Minnesota, School of Physics and Astronomy, Minneapolis, MN, USA, Michael Niemack ([email protected]) National Institute of Standards and Technology and University of Colorado, Boulder, CO, USA, and Lyman Page ([email protected]) Princeton University, Department of Physics, Princeton NJ, USA. March 26, 2012 Abstract The cosmic microwave background radiation (CMB) is now firmly established as a funda- mental and essential probe of the geometry, constituents, and birth of the Universe. The CMB is a potent observable because it can be measured with precision and accuracy. Just as importantly, theoretical models of the Universe can predict the characteristics of the CMB to high accuracy, and those predictions can be directly compared to observations. There are multiple aspects associated with making a precise measurement. In this review, we focus on optical components for the instrumentation used to measure the CMB polarization and temperature anisotropy. We begin with an overview of general considerations for CMB ob- servations and discuss common concepts used in the community. We next consider a variety of alternatives available for a designer of a CMB telescope. Our discussion is guided by arXiv:1206.2402v1 [astro-ph.IM] 11 Jun 2012 the ground and balloon-based instruments that have been implemented over the years. In the same vein, we compare the arc-minute resolution Atacama Cosmology Telescope (ACT) and the South Pole Telescope (SPT). CMB interferometers are presented briefly. We con- clude with a comparison of the four CMB satellites, Relikt, COBE, WMAP, and Planck, to demonstrate a remarkable evolution in design, sensitivity, resolution, and complexity over the past thirty years.
    [Show full text]
  • A Bit of History Satellites Balloons Ground-Based
    Experimental Landscape ● A Bit of History ● Satellites ● Balloons ● Ground-Based Ground-Based Experiments There have been many: ABS, ACBAR, ACME, ACT, AMI, AMiBA, APEX, ATCA, BEAST, BICEP[2|3]/Keck, BIMA, CAPMAP, CAT, CBI, CLASS, COBRA, COSMOSOMAS, DASI, MAT, MUSTANG, OVRO, Penzias & Wilson, etc., PIQUE, Polatron, Polarbear, Python, QUaD, QUBIC, QUIET, QUIJOTE, Saskatoon, SP94, SPT, SuZIE, SZA, Tenerife, VSA, White Dish & more! QUAD 2017-11-17 Ganga/Experimental Landscape 2/33 Balloons There have been a number: 19 GHz Survey, Archeops, ARGO, ARCADE, BOOMERanG, EBEX, FIRS, MAX, MAXIMA, MSAM, PIPER, QMAP, Spider, TopHat, & more! BOOMERANG 2017-11-17 Ganga/Experimental Landscape 3/33 Satellites There have been 4 (or 5?): Relikt, COBE, WMAP, Planck (+IRTS!) Planck 2017-11-17 Ganga/Experimental Landscape 4/33 Rockets & Airplanes For example, COBRA, Berkeley-Nagoya Excess, U2 Anisotropy Measurements & others... It’s difficult to get integration time on these platforms, so while they are still used in the infrared, they are no longer often used for the http://aether.lbl.gov/www/projects/U2/ CMB. 2017-11-17 Ganga/Experimental Landscape 5/33 (from R. Stompor) Radek Stompor http://litebird.jp/eng/ 2017-11-17 Ganga/Experimental Landscape 6/33 Other Satellite Possibilities ● US “CMB Probe” ● CORE-like – Studying two possibilities – Discussions ongoing ● Imager with India/ISRO & others ● Spectrophotometer – Could include imager – Inputs being prepared for AND low-angular- the Decadal Process resolution spectrophotometer? https://zzz.physics.umn.edu/ipsig/
    [Show full text]
  • The QMAP and MAT/TOCO Experiments for Measuring Anisotropy in the Cosmic Microwave Background
    Dartmouth College Dartmouth Digital Commons Dartmouth Scholarship Faculty Work 1-16-2002 The QMAP and MAT/TOCO Experiments for Measuring Anisotropy in the Cosmic Microwave Background A. Miller Princeton University J. Beach Princeton University S. Bradley Princeton University R. Caldwell Dartmouth College H. Chapman University of Pennsylvania See next page for additional authors Follow this and additional works at: https://digitalcommons.dartmouth.edu/facoa Part of the Astrophysics and Astronomy Commons Dartmouth Digital Commons Citation Miller, A.; Beach, J.; Bradley, S.; Caldwell, R.; Chapman, H.; Devlin, M. J.; Devlin, W. B.; Dorwart, W. B.; Herbig, T.; Jones, D.; Monnelly, G.; Netterfield, C. B.; Nolta, M.; Page, L. A.; Puchalla, J.; Robertson, T.; Torbet, E.; Tran, H. T.; and Vinje, W. E., "The QMAP and MAT/TOCO Experiments for Measuring Anisotropy in the Cosmic Microwave Background" (2002). Dartmouth Scholarship. 3442. https://digitalcommons.dartmouth.edu/facoa/3442 This Article is brought to you for free and open access by the Faculty Work at Dartmouth Digital Commons. It has been accepted for inclusion in Dartmouth Scholarship by an authorized administrator of Dartmouth Digital Commons. For more information, please contact [email protected]. Authors A. Miller, J. Beach, S. Bradley, R. Caldwell, H. Chapman, M. J. Devlin, W. B. Devlin, W. B. Dorwart, T. Herbig, D. Jones, G. Monnelly, C. B. Netterfield, M. Nolta, L. A. Page, J. Puchalla, T. Robertson, E. Torbet, H. T. Tran, and W. E. Vinje This article is available at Dartmouth Digital Commons: https://digitalcommons.dartmouth.edu/facoa/3442 The Astrophysical Journal Supplement Series, 140:115–141, 2002 June E # 2002.
    [Show full text]
  • THE ATACAMA Cosi'vl0logy TELESCOPE: the RECEIVER and INSTRUMENTATION L2 D
    https://ntrs.nasa.gov/search.jsp?R=20120002550 2019-08-30T19:06:35+00:00Z CORE Metadata, citation and similar papers at core.ac.uk Provided by NASA Technical Reports Server THE ATACAMA COSi'vl0LOGY TELESCOPE: THE RECEIVER AND INSTRUMENTATION L2 D. S. SWETZ , P. A. R. ADE\ j'vI. A !\fIRrl, J. \V'. ApPEL" E. S. BATTISTELLlfi,j, B. BURGERI, J. CHERVENAK', 2 lVI. J. DEVLIN], S. R. DICKER]. \V. B. DORIESE , R. DUNNER', T. ESSINGER-HILEMAN'. R. P. FISHER:', J. \V. FOWLER'. 4 2 1 lVI. HALPERN ,!.VI. HASSELFIELD4, G. C. HILTON , A. D. HINCKS\ K. D. IRWIN2. N. JAROSIK', M. KAlIL', J. KLEIN , . ull 11 I2 l l u 1 J. J\1. LAd "" M. LIMON , T. A. l'vIARRIAGE . D. MARSDEN , K. J\IARTOCCI : , P. J\IAUSKOPF: , H. MOSELEY', I4 2 C. B. NETTERFIELD , J\1. D. NIEMACK " l'vI. R. NOLTA ,L. A. PAGE". L. PARKER'. S. T. STAGGS", O. STRYZAK', 1 U jHi E. R. SWlTZER : , R. THORNTON • C. TUCKER'], E. \VOLLACK', Y. ZHAO" Draft version July 5, 2010 ABSTRACT The Atacama Cosmology Telescope was designed to measure small-scale anisotropies in the Cosmic Microwave Background and detect galaxy clusters through the Sunyaev-Zel'dovich effect. The instru­ ment is located on Cerro Taco in the Atacama Desert, at an altitude of 5190 meters. A six-met.er off-axis Gregorian telescope feeds a new type of cryogenic receiver, the Millimeter Bolometer Array Camera. The receiver features three WOO-element arrays of transition-edge sensor bolometers for observations at 148 GHz, 218 GHz, and 277 GHz.
    [Show full text]
  • Jeff Filippini
    The View from the Stratosphere Systematics and Calibration Challenges of CMB Ballooning Jeff Filippini CMB Systematics / Calibration Workshop 01Dec2020 Why Ballooning? The Good • High sensitivity to approach CMB photon noise limit • Access to higher frequencies obscured from the ground • Retain larger angular scales due to reduced atmospheric fluctuations (less aggressive filtering) • Technology pathfinder for orbital missions 101 100 The Bad -1 10 • Limited integration time (~weeks) 10-2 • Stringent mass, power constraints 10-3 • Very limited bandwidth demands 10-4 nearly autonomous operations Sky Radiance [pW/GHz] -5 10 1 km 10 km 30 km 101 102 103 A.S. Rahlin / am model Frequency [GHz] Excellent proxy for space operations! A Rich History BOOMERanG 1998 ARCADE 2 2006 SPIDER 2015 MAXIMA 1999 EBEX 2012 OLIMPO 2018 … plus BAM, QMAP, Archeops, TopHat, PIPER, and many more! Balloonatics The SPIDER Program A balloon-borne payload to identify primordial B-modes on degree angular scales in the presence of foregrounds Large (~1300L) shared LHe cryostat Modular: 6 monochromatic refractors • SPIDER 2015: 3x95 GHz, 3x150 GHz • SPIDER-2: 2x95, 1x150, 3x280 GHz Stepped half-wave plates (HWPs) Lightweight carbon fiber gondola Azimuthal reaction wheel, linear elevation drive Launch mass: ~6500 lbs (3000 kg) Nagy+ ApJ 844, 151 (2017) O’Dea+ ApJ 738, 63 (2011) Rahlin+ Proc. SPIE (2014) Filippini+ Proc. SPIE (2010) Fraisse+ JCAP 04 (2013) 047 … and more … SPIDER Receivers • Monochromatic 2-lens refractors Cold HDPE lenses, 264mm stop • Emphasis on low internal loading • Predominantly reflective filter stack Metal-mesh + one 4K nylon • Inter-lens 1.6K absorptive baffling • Thin vacuum window (3/32” UHMWPE) • Reflective wide-angle fore baffle • Polarization modulation with stepped cryogenic HWP (AR-coated sapphire) • Antenna-coupled TES arrays SPIDER-2: Horn-coupled TES arrays Challenges of CMB Ballooning Ballooning shares all of the same systematics and calibration challenges as anyone else - see e.g.
    [Show full text]
  • Cosmic Microwave Background Anisotropies Gravitational Secondaries
    1 Annu. Rev. Astron. and Astrophys. 2002 Parameter Sensitivity .................................... 26 BEYOND THE PEAKS ................................. 29 Matter Power Spectrum . .................................. 29 Cosmic Microwave Background Anisotropies Gravitational Secondaries .................................. 31 Scattering Secondaries .................................... 36 Non-Gaussianity . ...................................... 39 Wayne Hu1,2,3 and Scott Dodelson2,3 1Center for Cosmological Physics, University of Chicago, Chicago, IL 60637 DATA ANALYSIS . ................................... 40 .......................................... 2NASA/Fermilab Astrophysics Center, P.O. Box 500, Batavia, IL 60510 Mapmaking 41 .................................... 3Department of Astronomy and Astrophysics, University of Chicago, Chicago, IL 60637 Bandpower Estimation 44 Cosmological Parameter Estimation ............................ 46 DISCUSSION ....................................... 47 KEYWORDS: background radiation, cosmology, theory, dark matter, early universe 1INTRODUCTION The field of cosmic microwave background (CMB) anisotropies has dramatically ABSTRACT: Cosmic microwave background (CMB) temperature anisotropies have and will continue to revolutionize our understanding of cosmology. The recent discovery of the previously advanced over the last decade (c.f. White et al 1994), especially on its obser- predicted acoustic peaks in the power spectrum has established a working cosmological model: vational front. The observations have
    [Show full text]
  • INFLATION in 1090 Causally Disconnected Regions  /   105 !!!
    Quantum Origin of the Universe Structure V. Mukhanov ASC, LMU, München Blaise Pascal Chair, ENS, Paris Before 1990 The Universe expands Hubble law v r 1 r Hr t : : 13,7bil. years v H There exists background radiation with the temperature T 3K Penzias, Wilson 1965 There is baryonic matter: about 25% of 4He, D....heavy elements Dark Matter???? baryonic origin??? Large Scale Structure: clusters of galaxies! Filaments, Voids?????????????????????? After 90 - present COBE 1992 2.725K Blackbody Spectrum of the CMB Space-Bases experiments: Relikt-1, COBE, WMAP, Planck Balloon: Boomerang, Maxima, Archeops, EBEX, ARCADE, QMAP, Spider, TopHat Ground-based: ABS, ACBAR, ACT, AMI, APEX, APEX-SZ, ATCA BICEP, BICEP2, BIMA, CAPMAP, CAT, CBI, Clover, COSMOSOMAS, DASI, FOCUS, GUBBINS, Keck Array, MAT, OCRA, OVRO, POLARBEAR, QUaD, QUBIC, QUIET, RGWBT, Sakaatoon, SPT, TOCO, SZA, Tenerife, VSA Expanding Universe: Facts Today: The Universe is homogeneous and isotropic on scales from 300 millions up to 13 billions light-years There exist structure on small scales: Planets, Stars, Galaxies, Clusters of galaxies Superclusters .... There is 75%H , 25% He a nd heavy elements in very small amounts In past the Universe was VERY hot There exist Dark Matter and Dark Energy When the Universe was about 1000 times smaller, it was extremely homogeneous and isotropic in all scales 105 a 1 T a a When the Universe was 1000 times smaller its temperature was about 2725K Nucleosynthesis Recombination ??? Quark-gluon Neutrinos decoupling, phase transition Electron-Positron pairs annihilation ( 1 sek) 10-4 sec t 1010 Electro-weak phase transition Very homogeneous Inhomogeneous ??? INFLATION In 1090 causally disconnected regions / 105 !!! .
    [Show full text]
  • Observations of the Polarisation of the Anomalous Microwave Emission: a Review
    Hindawi Publishing Corporation Advances in Astronomy Volume 2012, Article ID 351836, 15 pages doi:10.1155/2012/351836 Review Article Observations of the Polarisation of the Anomalous Microwave Emission: A Review J. A. Rubino-Mart˜ ın,´ 1, 2 C. H. Lopez-Caraballo,´ 1, 2 R. Genova-Santos,´ 1, 2 and R. Rebolo1, 2 1 Instituto de Astrof´ısica de Canarias (IAC), C/V´ıa Lactea´ s/n, 38200 La Laguna, Tenerife, Spain 2 Departamento de Astrof´ısica, Universidad de La Laguna, 38206 La Laguna, Tenerife, Spain Correspondence should be addressed to J. A. Rubino-Mart˜ ´ın, [email protected] Received 13 August 2012; Accepted 10 October 2012 Academic Editor: Clive Dickinson Copyright © 2012 J. A. Rubino-Mart˜ ´ın et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. The observational status of the polarisation of the anomalous microwave emission (AME) is reviewed, both for individual compact Galactic regions as well as for the large-scale Galactic emission. There are six Galactic regions with existing polarisation constraints in the relevant range of 10–40 GHz: four dust clouds (Perseus, ρ Ophiuchi, LDN1622, and Pleiades) and two HII regions (LPH96 and the Helix nebula). These constraints are discussed in detail and are complemented by deriving upper limits on the polarisation of the AME for those objects without published WMAP constraints. For the case of large-scale emission, two recent works, based on WMAP data, are reviewed. Currently, the best constraints on the fractional polarisation of the AME, at frequencies near the peak of the emission (i.e., 20–30 GHz), are at the level of ∼ 1% (95.4% confidence level).
    [Show full text]
  • Aps2015wollack IPSIG Presentation.Pptx
    COSMIC MICROWAVE BACKGROUND POLARIZATION: STATUS AND EXPERIMENTAL PROSPECTS Edward J. Wollack Inflation Probe Science Interest Group (IPSIG) NASA Goddard Space Flight Center March 12, 2015 CMB: Past and Present… Planck (2009-present) WMAP (2001-2010) QUaD COBE (1989-1993) SPTpolAPEXSZ COBE MUSTANG2 BICEP2 Python SPIDER POLARBEARMAT SPOrt ACME FIRS CBI SZA BOOMERanG MBIB SK VSA QUIET TopHat PlanckMAXIMA QMASK MSAM AMI ACTPolHACME PIQUE Tenerife BAM EBEX BICEP BEAST ARCADE KECKArray ARGO BIMA TRIS COMPASS ACBAR CG DASI ATCAWMAP APACHE AMiBA QUIJOTE ABS ACTQMAP CLASS Clover CAT Archeops MINT KUPID PIPERSPT POLAR COSMOSOMAS Penzias & Wilson (1965) SuZIE CAPMAP Relikt MUSTANG Polatron CMB Physics: Temperature & Polarization • CMB blackbody radiation is anisotropic and polarized… • Temperature anisotropy à polarization via scattering • Powerful constraints on physics of the early Universe CMB Status: Temperature & Polarization • Planck – full sky maps with 4’ resolution available… • Rich cosmological and galactic data sets… • Consistency with 6 parameter cosmological model… • Consistency among numerous experiments… Planck Planck TE 2015 EE 2015 CMB Status: Temperature & Polarization ~ November 2014 L. Page CMB Status: Temperature & Polarization ~ March 2015 L. Page CMB Status: Temperature & Polarization • Temperature power spectra characterized over ~ four decades by a variety of experiments… • No surprises with E-mode power spectra… • Indirect detections of B-mode via lensing… • Joint BICEP2/Keck/Planck analysis limit on scalar to tensor ratio, r<0.12, at 95% confidence. Marginalizing over dust and r, lensing B-modes are detected at 7σ significance. Dust a significant foreground at 150GHz… P.A.R. Ade et al., “Joint Analysis of BICEP2/Keck Array and Planck Data” PRL (2015) 114, 101301.
    [Show full text]
  • The Cosmic Microwave Background & Inflation
    HTffiL ABSTRACT + LinKS The Cosmic Microwave Background & Inflation, Then & Now 1 1 2 3 4 J. Richard Bond , Carlo Contaldi , Dmitry Pogosyan , Brian Mason • , Steve Myers4, Tim Pearson3, Ue-Li Pen1, Simon Prunet5•1, Tony 3 3 Readhead , Jonathan Sievers 1. CJAR Cosmology Program, Canadian Institute for Theoretical Astrophysics, Toronto, Ontario, Canada 2. Physics Department, University of Alberta, Edmonton, Alberta, Canada 3. Astronomy Department, California Institute of Technology, Pasadena, California, USA 4. National Radio Astronomy Observatory, Socorro, New Mexico, USA 5. Institut d' Astrophysique de Paris, Paris, France Abstract. The most recent results from the Boomerang, Maxima, DASI, CBI and VSA CMB experiments significantly increase the case for accelerated expansion in the early universe (the inflationary paradigm) and at the current epoch (dark energy dominance). This is especially so when combined with data on high redshift supernovae (SNI) and large scale structure (LSS), encoding information from local cluster abundances, galaxy clustering, and gravitational lensing. There are "7 pillars of Inflation" that can be shown with the CMB probe, and at least 5, and possibly 6, of these have already been demonstrated in the CMB data: (I) the effects of a large scale gravitational potential, demonstrated with COBE/DMR in 1992-96; (2) acoustic peaks/dips in the angular power spectrum of the radiation, which tell about the geometry of the Universe, with the large first peak convincingly shown with Boomerang and Maxima data in 2000, a
    [Show full text]
  • Experimental CMB Status and Prospects: a Report from Snowmass 2001
    Experimental CMB Status and Prospects: A Report from Snowmass 2001 Suzanne Staggs Princeton University∗ Sarah Church Stanford University† (Dated: October 15th, 2001) In recent years the promise of experimental study of the cosmic microwave background (CMB) has been demonstrated. Herein a brief summary of the field is followed by an indication of future directions. The prospects for further revelations from the details of the CMB are excellent. The future work is well-suited to the interests of high energy physics experimentalists: the projects seek to understand the fundamental nature of the universe, require subtle experimental techniques to keep systematics in control, produce large, rich data sets, and must be implemented by multi-institutional collaborations. I. INTRODUCTION The vast cache of information encoded in the CMB’s intensity distribution has been tapped in recent years. In the last three years, a spate of independent experiments has evinced the primordial fluctuations present when the radiation decoupled from the matter at a redshift of z ≈ 1100. Continuing measurements of the CMB temperature anisotropy should soon be joined by measurements of its polarization anisotropy. The polarization presents the enticing possibility of educing information about the inflation field itself. A third exciting area of CMB research is the measurement of its fine-scale anisotropy, at ∼> 2500, where secondary effects dominate, so that the CMB serves as a backlight to illuminate dark parts of the universe. One of the main features of the fine-scale anisotropy is the Sunyaev-Zel’dovich effect in clusters, causing clusters to appear as either hot or cold spots, depending on the frequency of observation.
    [Show full text]
  • Toward a Mass-Limited Catalog of Galaxy Clusters from the Atacama Cosmology Telescope
    Toward a Mass-Limited Catalog of Galaxy Clusters from the Atacama Cosmology Telescope Adam Douglas Hincks ADISSERTATION PRESENTED TO THE FACULTY OF PRINCETON UNIVERSITY IN CANDIDACY FOR THE DEGREE OF DOCTOR OF PHILOSOPHY RECOMMENDED FOR ACCEPTANCE BY THE DEPARTMENT OF PHYSICS ADVISER:LYMAN A. PAGE,JR. SEPTEMBER 2009 c Copyright by Adam Douglas Hincks, 2009. All rights reserved. Abstract The Atacama Cosmology Telescope (ACT) is a six meter observatory in the Andes of northern Chile. It is currently in its third season of operation, observing the cosmic microwave background (CMB) with about 1000 detectors each at 148 GHz, 218 GHz, and 277 GHz. Capable of producing high sensitivity maps of the CMB at arcminute resolution, the ACT will contribute to our knowledge of cosmology by constraining the parameters describing the early universe as well as by studying its subsequent evolution. One of the more important tools for investigating the latter will be the Sunyaev-Zel’dovich (SZ) effect, by which large clusters of galaxies leave distinct imprints in the CMB, the strength of which is nearly independent of redshift. In this dissertation, we present maps of the first SZ clusters to be detected by the ACT, showing that we are beginning to reach our objective of creating a large, mass-limited catalog of clusters for probing the growth of structure in the universe. Extensive data analysis is required to produce our CMB maps, so, after describing the telescope itself, much of the dissertation is devoted to presenting some of the mapmaking elements. In particular, we have developed a pipeline which specializes at removing atmospheric contamination from the data to produce small, clean maps suitable for cluster analysis.
    [Show full text]