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Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Planets and Celestial Calibration Sources

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TLDR
In this article, seven-year observations of bright sources which are often used as calibrators at microwave frequencies were studied in five frequency bands (23 - 94 GHz): the outer planets (Mars, Jupiter, Saturn, Uranus and Neptune) and five fixed celestial sources (Cas A, Tau A, Cyg A, 3C274 and 3C58).
Abstract
(Abridged) We present WMAP seven-year observations of bright sources which are often used as calibrators at microwave frequencies. Ten objects are studied in five frequency bands (23 - 94 GHz): the outer planets (Mars, Jupiter, Saturn, Uranus and Neptune) and five fixed celestial sources (Cas A, Tau A, Cyg A, 3C274 and 3C58). The seven-year analysis of Jupiter provides temperatures which are within 1-sigma of the previously published WMAP five-year values, with slightly tighter constraints on variability with orbital phase, and limits (but no detections) on linear polarization. Scaling factors are provided which, when multiplied by the Wright Mars thermal model predictions at 350 micron, reproduce WMAP seasonally averaged observations of Mars within ~2%. An empirical model is described which fits brightness variations of Saturn due to geometrical effects and can be used to predict the WMAP observations to within 3%. Seven-year mean temperatures for Uranus and Neptune are also tabulated. Uncertainties in Uranus temperatures are 3%-4% in the 41, 61 and 94 GHz bands; the smallest uncertainty for Neptune is ~8% for the 94 GHz band. Intriguingly, the spectrum of Uranus appears to show a dip at ~30 GHz of unidentified origin, although the feature is not of high statistical significance. Flux densities for the five selected fixed celestial sources are derived from the seven-year WMAP sky maps, and are tabulated for Stokes I, Q and U, along with polarization fraction and position angle. Fractional uncertainties for the Stokes I fluxes are typically 1% to 3%. Source variability over the seven-year baseline is also estimated. Significant secular decrease is seen for Cas A and Tau A: our results are consistent with a frequency independent decrease of about 0.53% per year for Cas A and 0.22% per year for Tau A.

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Proceedings ArticleDOI

ACTPol: a polarization-sensitive receiver for the Atacama Cosmology Telescope.

TL;DR: The Atacama Cosmology Telescope (ACT) in Chile was built to measure the cosmic microwave background (CMB) at arcminute angular scales as discussed by the authors, and a new polarization sensitive receiver for ACT was proposed to characterize the gravitational lensing of the CMB and constrain the sum of the neutrino masses with ~ 0.05 eV precision.
Journal ArticleDOI

The Atacama Cosmology Telescope: A Measurement of the Cosmic Microwave Background Power Spectrum at 148 and 218 GHz from the 2008 Southern Survey

TL;DR: In this paper, the second through the seventh acoustic peaks in the CMB power spectrum were measured by the Atacama Cosmology Telescope at 148 GHz and 218 GHz, as well as the crossfrequency spectrum between the two channels.
Journal ArticleDOI

The Atacama Cosmology Telescope: CMB Polarization at $200<\ell<9000$

TL;DR: In this paper, the Atacama Cosmology Telescope Polarimeter (ACTPol) was used for measurements of the cosmic microwave background (CMB) and celestial polarization at 146 GHz made with the ACTPol in its first three months of observing.
References
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Journal ArticleDOI

Global spectral energy distribution of the Crab Nebula in the prospect of the Planck satellite polarisation calibration

TL;DR: In this paper, the spectral energy distribution (SED) of the Crab Nebula has been studied over more than 6 decades in frequency ranging from 1 to 10^6 GHz in the Planck satellite mission.
Posted Content

Infrared Brightness Temperature of Mars, 1983-2103

TL;DR: In this article, the predicted infrared brightness temperature of Mars using the 1976 model of Wright is tabulated for the period 1983 to 2103, and the model was developed for far-infrared calibration, and is still used for JCMT calibration.
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