CBI Observations of the Sunyaev-Zeldovich Effect

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Presentation transcript:

CBI Observations of the Sunyaev-Zeldovich Effect Steven T. Myers*, Patricia Udomprasert, and the CBI Team *National Radio Astronomy Observatory Socorro, NM

The Sunyaev-Zeldovich Effect

Behind clusters of galaxies is … A2597 Chandra, courtesy NASA/CXC/Ohio U/B.McNamara et al.

The Cosmic Microwave Background Discovered 1965 (Penzias & Wilson) 2.7 K blackbody Isotropic Relic of hot “big bang” 3 mK dipole (Doppler) COBE 1992 Blackbody 2.725 K Anisotropies 10-5

Thermal History of the Universe Courtesy Wayne Hu – http://background.uchicago.edu

The SZE The Sunyaev-Zeldovich Effect Compton upscattering of CMB photons by keV electrons decrement in I below CMB thermal peak (increment above) negative extended sources (absorption against 3K CMB) massive clusters mK, but shallow profile θ-1 → -exp(-v)                                    

CL 0016+16, z = 0.55 (Carlstrom et al.) X-Ray SZE:  = 15 K, contours =2

Sample from 60 OVRO/BIMA imaged clusters, 0.07 < z < 1.03

The Cosmic Background Imager

The Instrument 13 90-cm Cassegrain antennas 6-meter platform 78 baselines 6-meter platform Baselines 1m – 5.51m 10 1 GHz channels 26-36 GHz HEMT amplifiers (NRAO) Cryogenic 6K, Tsys 20 K Single polarization (R or L) Polarizers from U. Chicago Analog correlators 780 complex correlators Field-of-view 44 arcmin Image noise 4 mJy/bm 900s Resolution 4.5 – 10 arcmin

3-Axis mount : rotatable platform

CBI Operations Observing in Chile since Nov 1999 NSF proposal 1994, funding in 1995 Assembled and tested at Caltech in 1998 Shipped to Chile in August 1999 Continued NSF funding in 2002, to end of 2004 Chile Operations 2004-2005 pending proposal Telescope at high site in Andes 16000 ft (~5000 m) Located on Science Preserve, co-located with ALMA Now also ATSE (Japan) and APEX (Germany), others Controlled on-site, oxygenated quarters in containers access from San Pedro de Atacama (1.5 hrs away)

CBI Beam and uv coverage 78 baselines and 10 frequency channels = 780 instantaneous visibilities Frequency channels give radial spread in uv plane Baselines locked to platform in pointing direction Baselines always perpendicular to source direction Delay lines not needed Very low fringe rates (susceptible to cross-talk and ground) Pointing platform rotatable to fill in uv coverage Parallactic angle rotation gives azimuthal spread Beam nearly circularly symmetric CBI uv plane is well-sampled few gaps inner hole (1.1D), outer limit dominates PSF

CBI Calibration from WMAP Jupiter Old uncertainty: 5% 2.7% high vs. WMAP Jupiter New uncertainty: 1.3% Ultimate goal: 0.5%

Decontamination Ground emission removal Foreground radio sources Strong on short baselines, depends on orientation Differencing between main SZ field and lead/trail field pairs (9m to 16.5m in RA=2-4 deg) Foreground radio sources Located in NVSS at 1.4 GHz, VLA 8.4 GHz Measured at 30 GHz with OVRO 40m Background CMB dominant contaminant for arcmin-scale clusters! include as error component

The CBI SZE Program

The CBI SZE Sample led by Patricia Udomprasert (PhD. Thesis Caltech 2003) drawn from ROSAT (Ebeling et al. 1996, 1998; de Grandi et al. 1999; Boehringer et al. 2003) f 0.1-2.4keV > 1.0 x 10-11 erg cm-2 sec-1 z < 0.1 L 0.1-2.4keV > 1.13 x 1044 h-2 erg s-1 declination –70° < d < 24 ° 24 clusters accessible to CBI primary sample 15 most luminous detailed in Udomprasert, Mason, Readhead & Pearson (2004) preprint

Subsample 7 clusters covers a range of luminosities and cluster types

CBI SZE visibility function Xray: θ-3 (b ~ 2/3) SZE: θ-1 → -exp(-v) dominated by shortest baselines

A85 Forman et al. astro-ph/0301476 (left) Raw CBI Image (center) CLEAN source-sub CBI Image (right) CBI w/ROSAT A85 – cluster with central cooling flow, some signs of merger activity, subcluster to south

A399 (left) Raw CBI Image (center) CLEAN source-sub CBI Image (right) CBI w/ROSAT A399 – pair with A401

A401 (left) Raw CBI Image (center) CLEAN source-sub CBI Image (right) CBI w/ROSAT A401 – pair with A399, likely interacting now or in past, cooling flow disrupted?

A478 A478 – relaxed cooling flow cluster, X-ray cavities from AGN Chandra: Sun et al. astro-ph/0210054 (inner region + 1.4 GHz radio) (left) Raw CBI Image (center) CLEAN source-sub CBI Image (right) CBI w/ROSAT A478 – relaxed cooling flow cluster, X-ray cavities from AGN

A754 A754 – “prototypical” violent merger, significantly disturbed Chandra: Govoni et al. astro-ph/0401421 (left) Raw CBI Image (center) CLEAN source-sub CBI Image (right) CBI w/ROSAT A754 – “prototypical” violent merger, significantly disturbed

A1651 A1651 – dynamically relaxed cD cluster, unremarkable (left) Raw CBI Image (center) CLEAN source-sub CBI Image (right) CBI w/ROSAT A1651 – dynamically relaxed cD cluster, unremarkable

A2597 A2597 Chandra, courtesy NASA/CXC/Ohio U/B.McNamara et al. (left) Raw CBI Image (center) CLEAN source-sub CBI Image (right) CBI w/ROSAT A2597 – regular cD cluster with cooling flow, AGN in center (see raw image) with X-ray shadows in X-ray

SZE vs. X-rays: The Main Event gas density profiles: X-ray surface brightness: SZE surface brightness: dependence on parameters: DA ~ h-1 ne0 ~ h1/2 → DISZE ~ h-1/2

Results unweighted H0 = 67 +30–18 +13 –6 km/s/Mpc uncertainties dominated by CMB confusion based on older X-ray data…

Gastrophysics? “mergers” A85, A399/401, A754 A401 & A754 somewhat low, A399 very low (but uncertain) “cooling cores” A85, A478, A2597 A478 high, A2597 very high (but uncertain)

Error Budget CMB anisotropies – the dominant uncertainty density model – b models, some bias correction needed temperature profiles – assume isothermal, investigate deviations radio point sources – residuals small after using counts cluster asphericity – < 4%, could be worse in individual clusters clumpy gas distribution – <ne2 > / <ne>2 bias, substructure? peculiar velocities – no bias, 0.04% for even 1000 km/s! non-thermal Comptonization – unknown, model dependent

And the upshot is… Sample average H0 consistent with canonical value uncertainties dominated by CMB, then astrophysics is there significant scatter among clusters? finish the full sample! Gastrophysics not cosmology turn it around – what does scatter say about clusters? need to use latest Chandra & XMM-Newton data! What about the pesky CMB? more distant clusters better, CMB less on smaller scales measure CMB at SZE null (2mm)

CBI SZE Interferometry Issues First ACBAR Cluster Image: A3266 z=.0545 Tx=6.2 keV Lx=9.5x1044 Courtesy ACBAR group Analysis issues joint CBI & Xray modelfitting removal of CMB (e.g. mode projection?) substructure! more sensitivity on small scales… GBT! get GBT source measurements with new 30GHz system! do SZ with GBT! Other SZE experiments ACBAR at South Pole Carlstrom’s SZA and SPT big bolometer arrays on GBT, ACT subtract CMB by measuring at SZE null (e.g. ACBAR)

The SZE as a CMB Foreground

SZE Signatures in CMB Spectral distortion of CMB Mason et al. 2003, ApJ, 591, 540 Spectral distortion of CMB Dominated by massive halos (galaxy clusters) Low-z clusters: ~ 10’-30’ z=1: ~1’  expected dominant signal in CMB on small angular scales Amplitude highly sensitive to s8 pengjie map is 1.19 deg x 1.19 deg; color scale is dT/T=-2y A. Cooray (astro-ph/0203048) P. Zhang, U. Pen, & B. Wang (astro-ph/0201375)

SZE Angular Power Spectrum Goldstein et al. 2003, ApJ, 599, 773 [Bond et al. 2002, astro-ph/0205386] Smooth Particle Hydrodynamics (5123) [Wadsley et al. 2002] Moving Mesh Hydrodynamics (5123) [Pen 1998] 143 Mpc 8=1.0 200 Mpc 8=1.0 200 Mpc 8=0.9 400 Mpc 8=0.9 Dawson et al. 2002 Review SZ effect – expected crossover Use of simulations to predict power Description of simulations Parameters of simulations Scaling of power with parameters confirms s8to the 7 Power for s8=1 and s8=0.9

The CBI Collaboration Caltech Team: Tony Readhead (Principal Investigator), John Cartwright, Alison Farmer, Russ Keeney, Brian Mason, Steve Miller, Steve Padin (Project Scientist), Tim Pearson, Walter Schaal, Martin Shepherd, Jonathan Sievers, Pat Udomprasert, John Yamasaki. Operations in Chile: Pablo Altamirano, Ricardo Bustos, Cristobal Achermann, Tomislav Vucina, Juan Pablo Jacob, José Cortes, Wilson Araya. Collaborators: Dick Bond (CITA), Leonardo Bronfman (University of Chile), John Carlstrom (University of Chicago), Simon Casassus (University of Chile), Carlo Contaldi (CITA), Nils Halverson (University of California, Berkeley), Bill Holzapfel (University of California, Berkeley), Marshall Joy (NASA's Marshall Space Flight Center), John Kovac (University of Chicago), Erik Leitch (University of Chicago), Jorge May (University of Chile), Steven Myers (National Radio Astronomy Observatory), Angel Otarola (European Southern Observatory), Ue-Li Pen (CITA), Dmitry Pogosyan (University of Alberta), Simon Prunet (Institut d'Astrophysique de Paris), Clem Pryke (University of Chicago). The CBI Project is a collaboration between the California Institute of Technology, the Canadian Institute for Theoretical Astrophysics, the National Radio Astronomy Observatory, the University of Chicago, and the Universidad de Chile. The project has been supported by funds from the National Science Foundation, the California Institute of Technology, Maxine and Ronald Linde, Cecil and Sally Drinkward, Barbara and Stanley Rawn Jr., the Kavli Institute,and the Canadian Institute for Advanced Research.