2005
DOI: 10.1071/as04068
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Beam Size, Shape and Efficiencies for the ATNF Mopra Radio Telescope at 86–115 GHz

Abstract: Abstract:We present data characterising the performance of the Mopra Radio Telescope during the period 2000-2004, including measurements of the beam size and shape, as well as the overall beam efficiency of the telescope. In 2004 the full width half maximum of the beam was measured to be 36 ± 3 at 86 GHz, falling to 33 ± 2 at 115 GHz. Based on our observations of Jupiter we measured the beam efficiency of the Gaussian main beam to be 0.49 ± 0.03 at 86 GHz and 0.42 ± 0.02 at 115 GHz. Sources with angular sizes … Show more

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Cited by 177 publications
(218 citation statements)
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“…The Monolithic Microwave Integrated Circuit (MMIC) receiver covers the spectral range from 77 to 117 GHz and the 8-GHz bandpass of the MOPS was centred at 112.5 GHz to include these four isotopologues. The angular resolution of the Mopra beam size is 33 arcsec FWHM (Ladd et al 2005), and after the median filter convolution applied in the data reduction is around 35 arcsec in the final data set. The extended beam efficiency, η XB = 0.55 at 115 GHz, was also determined by Ladd et al This is used to convert brightness temperatures into line fluxes for determination of source parameters (rather than the main beam efficiency factor, of η MB = 0.42).…”
Section: Observationsmentioning
confidence: 99%
“…The Monolithic Microwave Integrated Circuit (MMIC) receiver covers the spectral range from 77 to 117 GHz and the 8-GHz bandpass of the MOPS was centred at 112.5 GHz to include these four isotopologues. The angular resolution of the Mopra beam size is 33 arcsec FWHM (Ladd et al 2005), and after the median filter convolution applied in the data reduction is around 35 arcsec in the final data set. The extended beam efficiency, η XB = 0.55 at 115 GHz, was also determined by Ladd et al This is used to convert brightness temperatures into line fluxes for determination of source parameters (rather than the main beam efficiency factor, of η MB = 0.42).…”
Section: Observationsmentioning
confidence: 99%
“…The references are: (a) Mookerjea et al (2004); (b) Becklin et al (1973); (c) Murphy et al (2010); (d) Figuerêdo et al (2005); (e) Breen et al (2007); (f) Caswell (1998); (g) Caswell et al (1995). Ladd et al (2005) and the beam efficiencies used are as listed there. The observing bandwidth was configured so that the central channel corresponded to −50 km s −1 , the approximate velocity at which the emission from the GMC complex is centred.…”
Section: Observations and Data Reductionmentioning
confidence: 99%
“…where T * A is the measured intensity and ην the beam efficiency (taken as 0.55 from Ladd et al (2005)). f is the beam filling factor for the emission, Jν (T ) = [hν/k]/[e (hν/kT ) − 1] with Tex being the excitation temperature and TBG being the temperature of the cosmic background radiation (i.e.…”
Section: Molecular Lines: Optical Depthsmentioning
confidence: 99%
“…Note that all spectra and Gaussian profile fitting are shown and performed on the T * A scale. To convert to main-beam brightness temperature (T mb ), the antenna temperature (T * A ) should be divided by the main-beam efficiency (η mb ) of 0.49 (Ladd et al 2005).…”
Section: Spectra Towards Each High-mass Clumpmentioning
confidence: 99%