2002
DOI: 10.1086/339498
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Understanding the Nature of Optically Faint Radio Sources and Their Connection to the Submillimeter Population

Abstract: We present a sample of 43 submillimeter sources detected (at >3 ) drawn from our program to follow up optically faint radio sources with the Submillimeter Common User Bolometric Array (SCUBA) instrument. These sources already have associated radio and, in many cases, optical identifications, and many are also detected at 450 lm. We compare these with 12 submillimeter sources drawn from the literature, which were discovered in blank-field mapping campaigns but also have radio detections. We then use this total … Show more

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Cited by 52 publications
(75 citation statements)
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“…If we propose that this local population of IR-luminous objects undergoes a strong luminosity evolution of the form ð1 þ zÞ 4 out to z ¼ 1:5, we can determine the relative numbers of cold and warm objects isolated by our selection function. This form of evolution has been shown to match the observe space density of high-z ULIRGs to the local population (see, e.g., Blain et al 1999;Chapman et al 2002a).…”
Section: Comparison With Higher Redshift Scuba Populationsmentioning
confidence: 73%
“…If we propose that this local population of IR-luminous objects undergoes a strong luminosity evolution of the form ð1 þ zÞ 4 out to z ¼ 1:5, we can determine the relative numbers of cold and warm objects isolated by our selection function. This form of evolution has been shown to match the observe space density of high-z ULIRGs to the local population (see, e.g., Blain et al 1999;Chapman et al 2002a).…”
Section: Comparison With Higher Redshift Scuba Populationsmentioning
confidence: 73%
“…Figure 12 illustrates both 850-870µm number counts (from Scuba, Laboca, Scuba-2, and ALMA Blain et al, 1999;Scott et al, 2002;Chapman et al, 2002;Cowie et al, 2002;Borys et al, 2003;Webb et al, 2003;Barnard et al, 2004;Coppin et al, 2006;Scott et al, 2006;Knudsen et al, 2008;Beelen et al, 2008;Weiß et al, 2009a;Karim et al, 2013;Casey et al, 2013;Chen et al, 2013a) and 450-500µm (from Scuba, Herschel and Scuba-2 Smail et al, 2002;Oliver et al, 2010;Clements et al, 2010;Béthermin et al, 2012b;Geach et al, 2013;Casey et al, 2013;Chen et al, 2013a). Figure 13 illustrates other infrared and submillimeter number counts in the literature in direct units, from 70µm Béthermin et al, 2010a;Berta et al, 2011), 100µm (Héraudeau et al, 2004;Rodighiero & Franceschini, 2004;Kawara et al, 2004;Berta et al, 2011;Magnelli et al, 2013b), 160µm Kawara et al, 2004;Béthermin et al, 2010a;Berta et al, 2011;Magnelli et al, 2013b), 250µm and 350µm Chen+13 (850) Casey+13 (850 Figure 12: Differential submillimeter number counts at 850µm/870µm (left) and 450-500 µm (right).…”
Section: Number Countsmentioning
confidence: 99%
“…Figure 13 illustrates other infrared and submillimeter number counts in the literature in direct units, from 70µm Béthermin et al, 2010a;Berta et al, 2011), 100µm (Héraudeau et al, 2004;Rodighiero & Franceschini, 2004;Kawara et al, 2004;Berta et al, 2011;Magnelli et al, 2013b), 160µm Kawara et al, 2004;Béthermin et al, 2010a;Berta et al, 2011;Magnelli et al, 2013b), 250µm and 350µm Chen+13 (850) Casey+13 (850 Figure 12: Differential submillimeter number counts at 850µm/870µm (left) and 450-500 µm (right). The 850µm and 870µm number counts come the initial Scuba surveys Scott et al, 2002;Chapman et al, 2002;Cowie et al, 2002;Borys et al, 2003;Webb et al, 2003;Barnard et al, 2004;Coppin et al, 2006;Scott et al, 2006;Knudsen et al, 2008, , shown in brown, dark red, red, dark orange, orange, dark gold yellow, light green, green, dark teal, and teal respectively). Data from Beelen et al (2008), Weiß et al (2009a), and Karim et al (2013) are taken at 870µm rather than 850µm, the two former from Laboca and the latter from interferometric ALMA data.…”
Section: Number Countsmentioning
confidence: 99%
“…A galaxy thus selected from this model universe is then assigned a template spectral energy distribution from the catalog of Dale et al (2001) and Dale & Helou (2002), parameterized by the 60=100 m color and normalized to the FIR luminosity. This model scenario does not incorporate the intrinsic scatter in the FIR /radio correlation (0.2 dex), as was done in Chapman et al (2002;hereafter C02). Rather, this study concentrates on the properties of the intrinsic dust temperature distribution, which locally shows a larger scatter (0.3 dex) than the FIR /radio correlation and should be expected to dominate the high-redshift radio and submillimeter properties.…”
Section: Fittinggthe Multiwavv Elengg Th Counts and Backgg Roundsmentioning
confidence: 99%