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Published bySuryadi Hermanto Modified over 5 years ago
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1.4 GHz Source Counts Melanie Gendre Walter Max-Moerbeck
Mitch Mickaliger Katie Rabidoux Under the supervision of Brian Mason and Jim Condon
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Overview Used GBT to measure continuum emission in a random patch of sky Calculated source counts Distribution of sources as function of flux density Large GBT beam size (9') can cause confusion Detection of a group of sources as one source
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Observations Used GBT (L-Band) 1410 MHz Continuum
Mapped 10º x 1º area 9' beam, Nyquist sampled Bonn 1420 MHz Survey Reich, 1982, A&AS48, 219. Reich and Reich, 1986, A&AS63, 205.
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Parameters Calibration source 3C286 G = 1.69 K/Jy FWHM = 9 arcmin
Effective Area = 4664 m^2 Aperture efficiency = 0.59 antenna solid angle = ^-6 srad mean beam solid angle = ^-6 srad mean beam efficiency = 0.55 Tsys = 14.5 K With an integration time of 0.2 s, and bandwidth of 50 MHz we get Tnoise = 4.6 mK Snoise = 2.71 mJy
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Reduction
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Results For a distribution of sources at a given flux density, the number of sources can be described by the power law n(S) = k * S-γ where k is a normalization constant and γ is the power law coefficient
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Results: Source Count {gamma, k}
{{1.7, }, {1.9, }, {2.1, }, {2.3, }} {S^2.5 n(s)} { , , , }
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