2000MNRAS.315..808S


Query : 2000MNRAS.315..808S

2000MNRAS.315..808S - Mon. Not. R. Astron. Soc., 315, 808-822 (2000/July-2)

An Australia Telescope survey for CMB anisotropies.

SUBRAHMANYAN R., KESTEVEN M.J., EKERS R.D., SINCLAIR M. and SILK J.

Abstract (from CDS):

We have surveyed six distinct `empty fields' using the Australia Telescope Compact Array (ATCA) in an ultracompact configuration with the aim of imaging, with a high brightness sensitivity, any arcminute-scale brightness-temperature anisotropies in the background radio sky. The six well-separated regions were observed at a frequency of 8.7GHz, and the survey regions were limited by the ATCA primary beams which have a full width at half-maximum of 6arcmin at this frequency; all fields were observed with a resolution of 2arcmin and an rms thermal noise of 24µJy.beam–1. After subtracting foreground confusion detected in higher resolution images of the fields, residual fluctuations in Stokes I images are consistent with the expectations from thermal noise and weaker (unidentified) foreground sources; the Stokes Q and U images are consistent with expectations from thermal noise.

Within the sensitivity of our observations, we have no reason to believe that there are any Sunyaev-Zeldovich holes in the microwave sky surveyed. Assuming Gaussian-form CMB anisotropy with a `flat' spectrum, we derive 95per cent confidence upper limits of Qflat<10-11µK in polarized intensity and Qflat<25µK in total intensity. The ATCA filter function peaks at l=4700 and has half-maximum values at l=3350 and 6050.


Abstract Copyright: Blackwell Science Ltd

Journal keyword(s): techniques: interferometric - cosmic microwave background - cosmology: observations - radio continuum: general

Simbad objects: 2

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Number of rows : 2
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 ClG 0016+16 ClG 00 18 33.3 +16 26 36           ~ 517 0
2 ICRF J193925.0-634245 Sy2 19 39 25.0245304992 -63 42 45.640373400   18.87 18.37 17.64   ~ 1332 2

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