Table 1
Details of the wavebands of the various single-dish observations used in this study.
Facility | Instrument | λ0 | ν0 | FWHM | ΩA | Bandwidth | Ccol |
---|---|---|---|---|---|---|---|
(μm) | (GHz) | (arcsec) | (10−9 sr) | (μm, GHz) | |||
Herschel | PACS | 70* | 4280 | 6.0a | – | 60–85c | 1.00 |
PACS | 160* | 1870 | 12.0a | – | 130–210c | 1.01 | |
SPIRE | 250* | 1200 | 18.0 | – | 211–290c | 1.02 | |
SPIRE | 350* | 857 | 24.0 | – | 297–405c | 1.01 | |
SPIRE | 500* | 600 | 35.0 | – | 409–611c | 1.03 | |
APEX | LABOCA | 869 | 345* | 19.2 | 12.17b | 313–372c | 0.988 |
IRAM | NIKA | 1153 | 260* | 12.0 | 4.51 | 196–273d | 0.971 |
30 m | NIKA | 1999 | 150* | 18.2 | 10.99 | 127–171d | 0.917 |
Notes. For the LABOCA and NIKA images, we detail the effective beam solid angles used to convert the images into units of MJy sr−1, though we note that the Hi-GAL images are supplied in units of MJy sr−1. The nominal wavelengths or frequencies recovered after colour correction are denoted in each case are denoted by an asterisk, and bandwidths are quoted in corresponding units. (a) We note that the 70 and 160 μm Hi-GAL images do not achieve the nominal beam size, but instead have PSFs that are elongated in the scan direction, and are measured to be 5.8′′ × 12.1′′ and 11.4′′ ×13.4′′, respectively. See Molinari et al. (2016) for more details. (b) We adopt the LABOCA total beam area for extended sources. See http://www.apex-telescope.org/bolometer/laboca/calibration/. (c) The PACS, SPIRE and LABOCA waveband edges are defined as half of the average in-band transmission (Siringo et al. 2009; Poglitsch et al. 2010; Swinyard et al. 2010). (d)The NIKA waveband edges contain ninety percent of the total transmission (Adam et al. 2014).
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