2009ApJ...694.1200R


Query : 2009ApJ...694.1200R

2009ApJ...694.1200R - Astrophys. J., 694, 1200-1219 (2009/April-1)

High-resolution CMB power spectrum from the complete ACBAR data set.

REICHARDT C.L., ADE P.A.R., BOCK J.J., BOND J.R., BREVIK J.A., CONTALDI C.R., DAUB M.D., DEMPSEY J.T., GOLDSTEIN J.H., HOLZAPFEL W.L., KUO C.L., LANGE A.E., LUEKER M., NEWCOMB M., PETERSON J.B., RUHL J., RUNYAN M.C. and STANISZEWSKI Z.

Abstract (from CDS):

In this paper, we present results from the complete set of cosmic microwave background (CMB) radiation temperature anisotropy observations made with the Arcminute Cosmology Bolometer Array Receiver (ACBAR) operating at 150 GHz. We include new data from the final 2005 observing season, expanding the number of detector hours by 210% and the sky coverage by 490% over that used for the previous ACBAR release. As a result, the band-power uncertainties have been reduced by more than a factor of two on angular scales encompassing the third to fifth acoustic peaks as well as the damping tail of the CMB power spectrum. The calibration uncertainty has been reduced from 6% to 2.1% in temperature through a direct comparison of the CMB anisotropy measured by ACBAR with that of the dipole-calibrated WMAP5 experiment. The measured power spectrum is consistent with a spatially flat, ΛCDM cosmological model. We include the effects of weak lensing in the power spectrum model computations and find that this significantly improves the fits of the models to the combined ACBAR+WMAP5 power spectrum. The preferred strength of the lensing is consistent with theoretical expectations. On fine angular scales, there is weak evidence (1.1σ) for excess power above the level expected from primary anisotropies. We expect any excess power to be dominated by the combination of emission from dusty protogalaxies and the Sunyaev-Zel'dovich effect (SZE). However, the excess observed by ACBAR is significantly smaller than the excess power at ℓ>2000 reported by the CBI experiment operating at 30 GHz. Therefore, while it is unlikely that the CBI excess has a primordial origin; the combined ACBAR and CBI results are consistent with the source of the CBI excess being either the SZE or radio source contamination.

Abstract Copyright: ∼

Journal keyword(s): cosmic microwave background - cosmology: observations

Simbad objects: 37

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Number of rows : 37
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 PMN J0018-4929 Rad 00 18 52.3475541375 -49 29 53.008682119           ~ 7 0
2 PMN J0026-5244 rG 00 26 47.86607 -52 44 15.2160           ~ 3 1
3 QSO B0047-5754 Bla 00 49 59.4728345616 -57 38 27.339177408   17.49 18.5 16.56   ~ 144 1
4 QSO B0056-572 Bla 00 58 46.5813154752 -56 59 11.469154272   17.91   16.95   ~ 98 1
5 AT20G J010333-643907 Bla 01 03 33.7430397768 -64 39 07.679028168       14.92   ~ 39 1
6 QSO B0122-514 Bla 01 24 57.39146099 -51 13 16.1675721   19.77   19.55   ~ 32 1
7 QSO B0131-522 Bla 01 33 05.76250002 -52 00 03.9454078   18.68 20.3 18.63   ~ 129 1
8 PMN J0144-6421 rG 01 44 16.76705 -64 21 42.7832       20.52   ~ 9 1
9 QSO B0208-512 BLL 02 10 46.2004407600 -51 01 01.893013392   17.10 16.93 14.82   ~ 485 1
10 ACT-S J022330-534737 Bla 02 23 30.8706976872 -53 47 39.875617392       19.07   ~ 20 1
11 PKS 0227-542 rG 02 29 12.78530889 -54 03 24.0345774           ~ 16 0
12 PMN J0231-6036 Rad 02 31 19.3 -60 36 57           ~ 4 1
13 QSO B0235-618 Bla 02 36 53.24574011 -61 36 15.1835463   18.18 18.5 17.62   ~ 117 1
14 QSO B0250-602 Bla 02 51 26.2467711216 -60 00 06.248999592     19.0 19.28   ~ 39 1
15 QSO B0252-549 Bla 02 53 29.1803201880 -54 41 51.437517216   17.65 19.3 16.79   ~ 141 1
16 PKS J0257-6112 rG 02 57 36.40797 -61 12 30.6507           ~ 9 1
17 QSO B0302-623 Bla 03 03 50.63135648 -62 11 25.5500344   19.48   17.87   ~ 159 1
18 QSO B0308-611 Bla 03 09 56.09914475 -60 58 39.0564095   19.00 18.5 18.18   ~ 154 1
19 QSO B0437-454 BLL 04 39 00.85466368 -45 22 22.5631875   20.44 20.6 19.48   ~ 121 1
20 QSO B0450-469 Bla 04 51 53.3468902656 -46 53 19.894609392   19.0 19.0     ~ 32 1
21 QSO B0454-463 Bla 04 55 50.77248730 -46 15 58.6797903   17.89 17.4 16.87   ~ 229 1
22 QSO B0514-459 Bla 05 15 45.2501347656 -45 56 43.198786536   18.18 17.5 17.31   ~ 132 1
23 PMN J0519-4546a Rad 05 19 35.08 -45 45 42.2           ~ 8 1
24 QSO B0524-433 Bla 05 25 54.8941429728 -43 18 01.299471192     18.0 19.3   ~ 18 2
25 QSO B0524-485 Bla 05 26 16.67131784 -48 30 36.7919695     20.0 19.36   ~ 107 1
26 9Y-MST J0531-4827 BLL 05 31 58.6155149088 -48 27 35.991354960           ~ 64 1
27 QSO B0537-441 BLL 05 38 50.36155950 -44 05 08.9390233   15.77 16.48 16   ~ 924 2
28 RCW 38 SFR 08 59 05.50 -47 30 39.4           ~ 327 2
29 QSO B2204-54 Bla 22 07 43.73329058 -53 46 33.8199643   18.45 18.0 18.20   ~ 178 1
30 PMN J2208-6404 Rad 22 08 19.6 -64 04 19           ~ 3 1
31 QSO B2232-488 Bla 22 35 13.23657823 -48 35 58.7945202   17.61 17.2     ~ 150 1
32 ICRF J223912.0-570100 QSO 22 39 12.07589936 -57 01 00.8395331       21.00   ~ 53 1
33 QSO B2243-563 Bla 22 46 16.79261972 -56 07 46.0059015   20.38   19.61   ~ 27 1
34 PMN J2309-5703 Rad 23 09 35.4 -57 03 51           ~ 3 1
35 ICRF J233444.9-525119 QSO 23 34 44.9165631576 -52 51 19.632336516   17.99   17.92   ~ 26 1
36 PKS J2336-5236 rG 23 36 12.14453637 -52 36 21.9510844   18.8       ~ 77 1
37 QSO B2355-534 BLL 23 57 53.26605016 -53 11 13.6895021   18.63 17.8 16.89   ~ 177 1

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