2013
DOI: 10.1093/mnras/stt1577
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The SCUBA-2 Cosmology Legacy Survey: demographics of the 450-μm population

Abstract: We investigate the multi-wavelength properties of a sample of 450-µm selected sources from the SCUBA-2 Cosmology Legacy Survey (S2CLS). A total of 69 sources were identified above 4σ in deep SCUBA-2 450-µm observations overlapping the UDS and COSMOS fields and covering 210 arcmin 2 to a typical depth of σ 450 = 1.5 mJy. Reliable cross identification are found for 58 sources (84 per cent) in Spitzer and Hubble Space Telescope WFC3/IR data. The photometric redshift distribution (dN/dz) of 450 µm-selected sources… Show more

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Cited by 41 publications
(51 citation statements)
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References 102 publications
(89 reference statements)
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“…It should be noted that this redshift distribution is significantly different than the distribution of either the 450 μm or 850 μm sources, who peak at z 1.95 0.19 450 á ñ =  and z 2.16 0.11 850 á ñ =  , respectively. The median of this parent distribution is z 1.46 0.14 á ñ =  , similar to the results of Roseboom et al (2013). We attribute this to the inclusion of the marginally detected 450 and 850 μm sources to our spectroscopic followup sample: these sources are less submillimeter luminous and so are likely at lower redshifts (see also Béthermin et al 2015).…”
Section: Photometric Redshift Analysissupporting
confidence: 75%
“…It should be noted that this redshift distribution is significantly different than the distribution of either the 450 μm or 850 μm sources, who peak at z 1.95 0.19 450 á ñ =  and z 2.16 0.11 850 á ñ =  , respectively. The median of this parent distribution is z 1.46 0.14 á ñ =  , similar to the results of Roseboom et al (2013). We attribute this to the inclusion of the marginally detected 450 and 850 μm sources to our spectroscopic followup sample: these sources are less submillimeter luminous and so are likely at lower redshifts (see also Béthermin et al 2015).…”
Section: Photometric Redshift Analysissupporting
confidence: 75%
“…The shapes of SEDs at the FIR wavelengths (λ 60 µm) are empirically found (e.g. Magnelli et al 2012;Casey et al 2013;Roseboom et al 2013) to be fairly well represented by a single modified blackbody function:…”
Section: Dust Propertiesmentioning
confidence: 93%
“…Such 450-µm-selected galaxies occupy similar parameter spaces to 850-µm sources in infrared luminosity (L IR ), SFR, and stellar mass, with typical ranges of 10 11.5 -10 13 L , 100-1000 M yr −1 , and 10 10.5 -10 11.5 M , respectively. However, 450-µm sources have dust temperatures higher than those of 850-µm sources by roughly 10 K Roseboom et al 2013). They are also at somewhat lower redshifts, with a peak of the redshift distribution at z = 1.5-2.0, Simpson et al 2014;Bourne et al 2017;Zavala et al 2018, cf.…”
Section: Introductionmentioning
confidence: 98%
See 1 more Smart Citation
“…The full detailed photometry is described in U et al (2012). The COSMOS sample includes the five-band Herschel 100-500 μm data, 24-70 μm Spitzer data, and, when available, AzTEC 1.1 mm data (Scott et al 2008;Aretxaga et al 2011) as well as Scuba-2 450 μm and 850 μm data Roseboom et al 2013). We use the far-infrared SED fitting technique described by Casey (2012); this has been shown to produce L IR , T dust and M dust estimates that are more accurate (when compared to direct interpolation of data) yet fully consistent with template fitting methods popular in the literature (e.g., Chary & Elbaz 2001;Dale & Helou 2002).…”
Section: Calculationsmentioning
confidence: 99%