2.6. Submm-wave selection effects
Deep submm-wave observations image the high-redshift
Universe with very little contamination from low-redshift
galaxies, and can potentially find a population of galaxies that is quite
different to those detected in conventional deep optical surveys, and which
could be undetectable in these surveys. The
complementarity of submm and optical observations is illustrated by
the very limited overlap between galaxies detected in the deep
submm-optical image shown in Fig. 1.
However, submm surveys are certainly subject to
selection effects. In Fig. 5
the flux-density-redshift relation for a submm-luminous
galaxy with a fixed bolometric luminosity is presented as a function of
its SED parameters - Td,
and
. The
relatively minor effects of different assumed cosmological models are
also shown. Changing the dust temperature has the greatest effect. The
inferred luminosity
of a dusty galaxy for a fixed observed submm flux density goes up by a
factor of 10 if the dust temperature is doubled, at all but the very
highest redshifts. There is thus a significant potential bias in
submm surveys against the detection of galaxies with
hotter dust temperatures for a given bolometric luminosity.
This effect was noted by Eales et al. (1999), when investigating the evolution of galaxies in the context of the results of deep SCUBA surveys. They suggested that the submm galaxies may be cooler than the temperatures of about 60 K usually assumed, and so their significance as a population of strongly evolving high-redshift galaxies may have been overestimated.
As discussed in Section 2.3, a cooler dust temperature of 40 K is compatible with observations of the SEDs of individual submm galaxies with confirmed redshifts detected in submm surveys (Ivison et al., 1998a, 2000a) and with the results of targeted observations of luminous low-redshift IRAS galaxies and high-redshift QSOs. If this temperature is assumed, then the inferences about galaxy evolution made from the results of submm surveys (Blain et al., 1999b, c; Eales et al., 2000; Smail et al., 2002) should be reliable. However, until a large sample of submm galaxies with redshifts and multi-waveband SEDs is available, the possibility that a cold or hot population of high-redshift dusty galaxies could be missing from or misidentified in submm surveys cannot be ruled out (Eales et al., 1999; Blain and Phillips, 2002). The possible effects on inferred luminosities of different forms of the SED shown in Fig. 5 need to be taken seriously, especially when describing the properties of individual galaxies selected in submm surveys.
There is little reliable evidence for a systematic relationship between dust temperature and redshift. Observations of low-redshift IRAS galaxies (Andreani and Franceschini, 1996; Dunne et al., 2000), indicate that any variation of dust temperature with luminosity appears to be gradual. However, there is evidence for a significant and systematic change in the temperature of dusty galaxies with a wider range of luminosities, from about 20 K for low-redshift spirals (Reach et al., 1995; Alton et al., 2000; Dunne and Eales, 2001) to about 40 K for more luminous objects typical of the galaxies detected in the IRAS survey. Temperatures of up to 110 K are found for some extremely luminous high-redshift galaxies (Lewis et al., 1998).
We stress that there could be a significant selection effect in submm surveys that depends on the range of dust temperatures in the source population. The importance of such an effect can be quantified once a complete redshift distribution is available for a submm-selected galaxy sample.