BLAST 250{\bf\rm\mu m} galaxies in GOODS-South

The BLAST 250-selected galaxy population in GOODS-South

J. S. Dunlop, P. A. R. Ade, J. J. Bock, E. L. Chapin, M. Cirasuolo, K. E. K. Coppin, Email:    M. J. Devlin, M. Griffin, T. R. Greve, J. O. Gundersen, M. Halpern, P. C. Hargrave,    D. H. Hughes, R. J. Ivison, J. Klein, A. Kovacs, G. Marsden, P. Mauskopf,    C. B. Netterfield, L. Olmi, E. Pascale, G. Patanchon, M. Rex, D. Scott,    C. Semisch, I. Smail, T. A. Targett, N. Thomas, M. D. P. Truch, C. Tucker,    G. S. Tucker, M. P. Viero, F. Walter, J. L. Wardlow, A. Weiss, D. V. Wiebe

SUPA, Institute for Astronomy, University of Edinburgh, Royal Observatory, Edinburgh, EH9 3HJ, UK
Department of Physics & Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, BC V6T 1Z1, Canada
School of Physics & Astronomy, Cardiff University, 5 The Parade, Cardiff, CF24 3AA, UK.
Jet Propulsion Laboratory, Pasadena, CA 91109-8099, USA.
Institute for Computational Cosmology, Durham University, South Road, Durham, DH1 3LE, UK.
Department of Physics & Astronomy, University of Pennsylvania, 209 South 33rd Street, Philadelphia, PA, 19104, USA.
Max-Planck Institut fur Astronomie, Konigstuhl 17, 69117 Heidelberg, Germany.
Department of Physics, University of Miami, 1320 Campo Sano Drive, Coral Gables, FL 33146, USA.
Instituto Nacional de Astrofísica Óptica y Electrónica (INAOE), Aptdo. Postal 51 y 72000 Puebla, Mexico.
UK ATC, Royal Observatory, Edinburgh, EH9 3HJ, UK
Max-Planck Institut fur Radioastronomy, Auf dem Hugel 69, 53121 Bonn, Germany.
Department of Astronomy & Astrophysics, University of Toronto, 50 St. George Street Toronto, ON M5S 3H4, Canada.
Department of Physics, University of Toronto, 60 St. George Street, Toronto, ON M5S 1A7, Canada.
University of Puerto Rico, Rio Piedras Campus, Physics Dept., Box 23343, UPR station, Puerto Rico.
IRA-INAF, Largo E. Fermi 5, I-50125, Firenze, Italy.
Laboratoire APC, 10, rue Alice Domon et Léonie Duquet 75205 Paris, France.
Department of Physics, Brown University, 182 Hope Street, Providence, RI 02912, USA.
Scottish Universities Physics Alliance
Accepted … ; Received … ; in original form …

We identify and investigate the nature of the 20 brightest 250  sources detected by the Balloon-borne Large Aperture Submillimetre Telescope (BLAST) within the central 150 arcmin of the GOODS-South field. Aided by the available deep VLA 1.4 GHz radio imaging, reaching (4-), we have identified radio counterparts for 17/20 of the 250  sources. The resulting enhanced positional accuracy of  arcsec has then allowed us to exploit the deep optical (HST), near-infrared (VLT) and mid-infrared (Spitzer) imaging of GOODS-South to establish secure galaxy counterparts for the 17 radio-identified sources, and plausible galaxy candidates for the 3 radio-unidentified sources. Confusion is a serious issue for this deep BLAST 250  survey, due to the large size of the beam. Nevertheless, we argue that our chosen counterparts are significant, and often dominant contributors to the measured BLAST flux densities. For all of these 20 galaxies we have been able to determine spectroscopic (8) or photometric (12) redshifts. The result is the first near-complete redshift distribution for a deep 250 -selected galaxy sample. This reveals that 250  surveys reaching detection limits of  mJy have a median redshift , and contain not only low-redshift spirals/LIRGs, but also the extreme dust-enshrouded starburst galaxies previously discovered at sub-millimetre wavelengths. Inspection of the LABOCA 870  imaging of GOODS-South yields detections of of the proposed BLAST sources (all at ), and reveals 250/870  flux-density ratios consistent with a standard 40 K modified black-body fit with a dust emissivity index . Based on their IRAC colours, we find that virtually all of the BLAST galaxy identifications appear better described as analogues of the M82 starburst galaxy, or Sc star-forming discs rather than highly obscured ULIRGs. This is perhaps as expected at low redshift, where the 250  BLAST selection function is biased towards spectral energy distributions which peak longward of . However, it also appears largely true at .

galaxies: active – galaxies: starburst – galaxies: photometry – galaxies: fundamental parameters – infrared: galaxies.
pagerange: 000–000

1 Introduction

The observed far-infrared background peaks around a wavelength (Puget et al. 1996; Fixsen et al. 1998). Over the past 10 years, deep extragalactic surveys have closed in on this wavelength regime from both shorter and longer wavelengths, and there has been dramatic progress in uncovering populations of sources which undoubtedly contribute to this background. Specifically, at wavelengths times longer than the peak (), surveys with the Sub-millimetre Common-User Bolometer Array (SCUBA), Mambo, AzTEC and now LABOCA (e.g. Coppin et al., 2006; Bertoldi et al. 2007; Weiss et al. 2009; Austermann et al. 2010) have been used to successfully assemble substantial samples of submm-selected extragalactic sources, and the spectral energy distributions (SEDs) of these sources are certainly rising steeply towards shorter wavelengths. Conversely, at wavelengths times shorter than the peak, the Spitzer Space Telescope has proved effective at extragalactic source selection up to wavelengths (Magnelli et al., 2009). But until now, the effective production of deep extragalactic samples in the central wavelength range has been prohibited by the atmosphere and/or limitations on instrument sensitivity and telescope aperture.

This situation should shortly be transformed by the SPIRE instrument on the 3.5-m diameter Herschel Space Observatory (Griffin et al. 2007). However, a powerful first insight into the nature of the -selected galaxy population is already being provided by the the Balloon-borne Large Aperture Submillimetre Telescope (BLAST).

BLAST is a 1.8 m diameter stratospheric balloon telescope that operates at an altitude of approximately 35 km, above most of the atmospheric water vapour which essentially prohibits effective far-infrared observations from the ground. BLAST is thus half the size of Herschel, and it is equipped with a camera which is a prototype of the SPIRE camera, enabling simultaneous broad-band imaging with central wavelengths of 250, 350 and 500 . In 2006, BLAST undertook an 11-day flight from Antarctica, during which it executed an observing programme which included the first deep far-infrared imaging survey ever undertaken within the Extended Chandra Deep Field South (ECDFS).

This unique survey (described in more detail in Section 2) has already been the subject of several investigations. First results on the far-infrared number counts and the resolution of the background were presented by Devlin et al. (2009), with more detailed investigations of these two key topics being presented by Patanchon et al. (2009) and Marsden et al. (2009). Pascale et al. (2009) used the survey to constrain cosmic star-formation history, while Viero et al. (2009) studied correlations in the background. Dye et al. (2009) and Ivison et al. (2010) used the supporting radio (VLA) and mid-infrared Spitzer imaging of the field to attempt to identify countparts to the brighter BLAST sources, and to explore the far-infrared/radio correlation in distant galaxies.

The study by Dye et al. (2009) showed that the BLAST beam, at least at , is still small enough to allow the successful identification of a reasonable fraction of BLAST sources with radio and mid-infrared counterparts. However, the supporting data over the full 9 deg BLAST survey area are of variable quality, and Dye et al. attempted to secure identifications for sources selected at all 3 BLAST wavelengths. As a result, they succeeded in identifying counterparts for only % of the sources in the BLAST catalogues detected at in at least one waveband. This inevitably limits the conclusions that can be drawn about the redshift distribution of the BLAST source population, although Dye et al. concluded that % of the sources in the shallow+deep catalogue lie at .

The aim of the study presented here is to establish a near-complete redshift distribution for a subset of the BLAST sources selected down to a fainter flux-density limit of  mJy, and subsequently to establish the basic physical properties (stellar mass, size, morphology, star-formation history, AGN content) of the galaxies which host the observed emission. To try to achieve this, we have deliberately confined our attention to the small sub-area of the BLAST map which contains the very best optical (HST ACS), near-infrared (VLT ISAAC) and mid-infrared (Spitzer) imaging data, and the highest density of optical spectroscopic redshifts. This area, the  arcmin GOODS-South field (Dickinson et al. 2004), is also where the radio (VLA) imaging is most sensitive, and it has been mapped in its entirety at by LABOCA (Weiss et al. 2009), and at 1.1 mm by AzTEC (Scott et al. 2010). GOODS-South is also the chosen location for some of the first deep high-resolution near-infrared imaging currently being undertaken with WFC3 on the refurbished HST, and is the future target of planned deep sub-mm and far-infrared imaging with SCUBA2 (Holland et al. 2006) and SPIRE+PACS on Herschel.

Thus, by confining our attention to GOODS-South we can explore just what can be achieved given the best possible supporting data. Conversely, we can also establish what level of supporting data is actually required for an effective, complete study of the future, larger, -selected galaxy samples which will be produced by Herschel. In addition, the wealth of existing information on other galaxy populations in this field (see Section 2) facilitates the comparison of BLAST galaxies with reference samples of field galaxies selected at similar redshifts and/or stellar masses, and to explore the frequency of mergers. Finally, the recent acquisition of deep sub-millimetre and millimetre wavelength imaging in the same field allows a first exploration of how the and populations are related.

To assemble a useful sample of sources within this field, we have pushed the BLAST source selection significance threshold to . However, the resulting sample is still sufficiently small (20 sources) that we can afford to explore the properties of individual sources in some detail. As a result this work should be regarded as a pilot study of the mix of source populations which can be uncovered in a deep survey, and an exploration of how best to overcome the problems that are encountered in trying to identify and study the faint far-infrared sources in maps which are inevitably highly confused (note that the Herschel beam at is essentially the same size as the BLAST beam at ). The broader statistical robustness of the results presented here is clearly limited both by small number statistics, and by cosmic variance.

The layout of the paper is as follows. In Section 2 we describe the selection and robustness of the BLAST sub-sample within the central region of GOODS-South, and then summarize the wealth of available multi-frequency imaging and spectroscopy in the field. In Section 3 we describe the process of obtaining radio and optical counterparts for the BLAST sources, and highlight the care required to overcome the problems associated with source blending in the confused BLAST maps. In Section 4 we provide or derive redshifts for all of the sources, including secondary/alternative counterparts. Then, in Section 5, we present multi-colour images of the BLAST galaxies and provide notes on each of the individual sources. Finally, in Section 6 we review our results and discuss the robustness of our conclusions. In particular we present and discuss the implications of the striking associations found between the BLAST sources and the LABOCA sources recently uncovered by Weiss et al. (2009). We also discuss the robustness of our derived redshift distribution for -selected sources, and briefly compare the mid-infrared colours of BLAST galaxies with those of other known galaxies at both high and low redshifts. Our conclusions are summarized in Section 7.

2 Data

Figure 1: The location of the 20 BLAST 250  sources in GOODS-South superimposed on the HST ACS -band imaging mosaic of the field (LH plot) and on a greyscale of the BLAST 250  map itself (RH plot). Sources are numbered by BLAST source ID (from the full BLAST map), as given in Table 1, with higher numbers indicating lower 250  flux densities. The circles have a radius of 15 arcsec, which is the radius adopted for the search for radio and optical counterparts to the BLAST sources. The actual BLAST beam has a FWHM of 36 arcsec at 250 


2.1 The BLAST 250  source sub-sample

The 250  source sample selected for study here represents a small subset of the far-infrared (250 , 350 , 500 ) sample uncovered in the ECDFS by the BLAST Antarctic flight of December 2006 (Devlin et al. 2009). An area of 8.7  centred on , (J2000) was mapped by BLAST to mean sensitivities of mJy, mJy, and mJy per beam. Within this ‘BLAST GOODS South Wide’ (BGS-Wide) map, a deeper image, reaching mJy, mJy, and mJy per beam was made of the central 0.8 centred on the southern field of the Great Observatories Origins Deep Survey (GOODS; Dickinson et al. 2003) at , (J2000). It is from the core of this ‘BLAST GOODS South Deep’ (BGS-Deep) map that we have extracted a ‘complete’ sub-sample of the BLAST 250  sources which lie within the sub-region with the very best supporting multi-frequency data. As shown in Fig. 1, we have chosen to define this area as the sq. arcmin region of sky covered by the GOODS-South HST ACS 4-band optical imaging (Giavalisco et al. 2004).

Because our primary aim here is to study the optical/infrared galaxy counterparts of the BLAST sources, we have confined our attention to 250  sources, because the larger BLAST beam sizes at 350 and 500  make it even more difficult to reliably identify all but the brightest longer-wavelength sources (the BLAST06 beams are best fit by Gaussians with FWHM of 36, 42, and 60 arcsec at 250 , 350  and 500  respectively; Pascale et al. 2008). Our study thus differs from, and complements that of Dye et al. (2009), who sought identifications for all 351 BLAST sources detected at in any one of the three BLAST wavebands across the whole of BLAST GOODS South survey. We have also extracted a significantly deeper sub-sample of sources for study, selecting all 250  sources which lie within the region shown in Fig. 1 and have a signal:noise ratio greater than 3.25. Pushing the BLAST data in this way allows us to construct a sample of useful size from within the relatively small area covered by the highest quality supporting datasets, and also allows a first investigation of the nature of the fainter 250  source population which will be studied in detail by Herschel.

Imposing this signal:noise cut produced a sample of 24 sources. We chose this significance threshold because, below this level, there are only 9 sources with signal:noise 2, and only three of these were reproduced at in an alternative map reduction (and all three at ). In other words, this threshold appears to mark a clear (not unexpected) point below which source reliability degenerates markedly, at least in this particular region of the BLAST map.

Of these 24 sources, we then rejected three (176, 228, 777) as inappropriate for this study because their nominal positions moved by greater than 20 arcsec between different map reductions. This does not necessarily mean these sources are not real peaks in the map (they range in S/N from 5 to 3.5), but simply that their positions appear to be too sensitive to the precise choice of map-production/source-extraction parameters to allow reliable determination of the most likely radio or optical counterpart (possibly because they are extreme examples of confusion from a number of fainter sources). There certainly appears to be something different about these sources because all other sources in our sample moved by less than 5 arcsec between alternative map reductions. Finally, we also rejected the second least significant source (1158), because it was not found at in the alternative map reduction.

This leaves a ‘clean’ sample of 20 sources for further study. The 250  positions of the BLAST sources are indicated in Fig. 1, and tabulated in Table 1, along with their 250  flux densities and signal:noise ratios. Given that the 4 rejected sources displayed a range of 250 signal:noise, the remaining sample can be regarded as representative down to a flux-density detection limit of in the zero-mean map ( relative to the local background – see below). The mean signal:noise ratio for these 20 sources is 5.6, but this is biased by the brightest 2 or 3 sources. The median signal:noise is 4.2, and this number is adopted as representative where appropriate later in this paper.

Before searching for identifications, it is worth pausing to consider the robustness of the far-infrared sources listed in Table 1.

The 250  flux densities given in Table 1 are the ‘raw’ values as extracted from the BLAST map via convolution with the relevant noise-weighted point-spread function (Truch et al 2009), effectively a weighted fit of the beam to the raw unsmoothed data to derive the best (maximum likelihood) estimate of the flux density of a point source in the map (e.g. Serjeant et al. 2003). Due to the steepness of the 250  source counts, and the large BLAST beam, the flux densities of the individual sources (which would be seen in a higher resolution map) will undoubtedly have been boosted by the effects of confusion (i.e. flux contributions from fainter sources) and by Eddington bias (a combination of noise and steep source counts), especially for the lower signal:noise detections (Scott et al. 2002; Coppin et al. 2006; Pantachon et al. 2009). Reading fluxes from the zero-mean map can, however, partially offset the flux contributions from fainter confused sources, which in effect constitute the local background for any brighter source in the map. However, detailed simulations are clearly required to establish robust statistical corrections for sources at a given flux density (Patanchon et al. 2009).

The other issue to consider is the noise. The flux-density noise levels quoted in Table 1 include only the instrumental noise which, within this deep section of the map, is typically  mJy per beam. However, analysis of the pixel flux-density distribution within the relevant 150 arcmin region under study here, shows that the spatial noise in the map is  mJy per beam (as measured from a Gaussian fit to the negative tail of the flux-density distribution). This implies that the confusion noise is comparable to the instrumental noise, at  mJy per beam. The situation is therefore similar to that encountered with the deepest 850  maps made of the Hubble Deep Field with SCUBA on the JCMT (Hughes et al. 1998; Peacock et al. 2000).

It might therefore seem appropriate to increase the noise level to  mJy per beam when assessing the significance of our sources in the actual map. However, if we choose to do this, for consistency we must also adopt the local background in the map which examination shows to be typically  mJy per beam. This is not surprising, as the mode of the distribution of flux-density values in the zero-mean map lies at  mJy per beam. Thus, performing aperture photometry on the map typically increases flux-densities by  mJy per beam, and boosts the assumed noise level to  mJy per beam. Adoption of these two corrections reduces only slightly the formal significance level of the sources listed in Table 1, and still leaves our faintest source above the 3 threshold.

Given these complications, in this paper we make little direct use of the 250  flux densities, other than to discuss the use of 250/870  flux-density ratio as a consistency check on derived source redshift (see Section 6.1). We also do not attempt to exploit the 350 or 500  measurements of our 250 -selected sources, as the larger beams, and relatively low sensitivity (at least to 250 -selected sources) of BLAST at these longer wavelengths prohibits the extraction of usefully accurate flux densities. We thus do not quote 350 or 500  flux densities for the sources in Table 1 (although values for the brighter sources can be found in Dye et al. 2009). We do, however, check, on a source-by-source basis, for detections or non-detections at these longer wavelengths, as described in Section 5. Finally, we note that as there are BLAST 250  beams in the 150 arcmin area under study here, we would expect non-existent sources to clear our adopted 3.3 threshold purely by chance. Relative to the 250  map mode of  mJy, the MUSIC region under study here contains one 3 negative peak. We thus conclude that, while flux boosting may be substantial for individual sources, our adopted signal:noise threshold is reasonable.

(IAU) ID (J2000) (J2000) (250) /mJy
BLAST J033235275530 () 4 53.146220 27.925272 16.2 177
BLAST J033229274414 () 6 53.123900 27.737326 14.4 157
BLAST J033218275216 () 59 53.075139 27.871343 6.7 74
BLAST J033205274645 () 66 53.022647 27.779397 6.6 72
BLAST J033235274932 () 104 53.147540 27.825642 6.0 65
BLAST J033217275054 () 109 53.072586 27.848349 5.9 64
BLAST J033221275630 () 158 53.088715 27.941911 5.2 58
BLAST J033212274642 () 193 53.051434 27.778541 4.9 54
BLAST J033217274944 () 257 53.073511 27.829046 4.6 51
BLAST J033242275514 () 318 53.176619 27.920633 4.4 48
BLAST J033238274954 () 503 53.159514 27.831733 4.0 44
BLAST J033213274302 () 552 53.054825 27.717303 3.9 43
BLAST J033247275418 () 593 53.197956 27.905028 3.9 43
BLAST J033243275146 () 637 53.181931 27.862863 3.8 42
BLAST J033232275304 () 654 53.136852 27.884531 3.8 42
BLAST J033243274650 () 732 53.179377 27.780768 3.7 40
BLAST J033213274246 () 830 53.056853 27.712811 3.6 40
BLAST J033248274443 () 861 53.200852 27.745501 3.6 39
BLAST J033232274558 () 983 53.134915 27.766112 3.4 38
BLAST J033246275321 () 1293 53.193438 27.889410 3.3 36
Table 1: The BLAST 250 -selected sample in GOODS-South. The positions are derived from optimal beam fitting to the BLAST map. is the flux density derived from the zero-mean BLAST map.

2.2 Supporting multi-frequency data

2.2.1 Radio: VLA 1.4-GHz imaging

As demonstrated by the follow-up of sub-millimetre surveys with SCUBA, very deep VLA imaging is necessary (and frequently sufficient) for the successful identification of the galaxy counterparts of sources detected with the large beams of current far-infrared/sub-millimetre facilities (e.g. Ivison et al. 2002, Ivison et al. 2007). This works for three reasons. First, star-forming galaxies produce copious quantities of synchrotron emission. Second, even in the deepest available radio maps, 1.4 GHz sources still have sufficiently low surface-density that positional coincidences within a ‘reasonable’ search radius are generally statistically rare. Third, if a robust radio counterpart is found, the arcsec positional accuracy provided by the VLA at GHz essentially always yields an unambiguous optical/infrared galaxy counterpart for further study.

Very deep (), high-resolution 1.4 GHz imaging of GOODS-South is now available at the centre of the ECDFS as described by Kellermann et al. (2008) and Miller et al. (2008). As discussed by Dye et al. (2009), the published source catalogue adopts a very conservative detection threshold of 7. We therefore re-analysed the image of Miller et al. (2008) using the techniques described by Ibar et al. (2009) to create a radio catalogue down to a limit of 30  (at which depth the cumulative source density on the sky is ). This catalogue was then searched for potential radio counterparts to the BLAST sources using the method described below in Section 3.

In cases where the radio emission appears heavily resolved (e.g. for the brightest source, BLAST 4, where at first sight there appear to be 6 individual VLA candidate counterparts) we measured the total radio flux density using TVSTAT within AIPS. We checked these values against the flux densities measured with the 16-arcsec beam of the Australia Telescope Compact Array (ACTA) (Norris et al. 2006), and found them to be in good agreement for the 4 sources which proved sufficiently bright to have also been detected at 1.4 GHz by ACTA (Afonso et al. 2006).

2.2.2 Optical: HST ACS imaging

Deep optical imaging over the 150 arcmin area shown in Fig. 1 has been obtained with the Advanced Camera for Surveys (ACS) on board HST in 4 different filters: , , and . These data were taken as part of GOODS (Giavalisco et al. 2004) and reach 5  limiting (AB) magnitudes (within a 1 arcsec diameter aperture) of 26.9, 26.9, 26.1, and 25.8, respectively. By definition, all 20 of the BLAST sources lie within the area covered by the GOODS-South HST ACS optical imaging. One of the BLAST sources (BLAST 732) lies within the even deeper ACS imaging provided by the Hubble Ultra Deep Field (HUDF: Beckwith et al. 2006), over an area of 11 arcmin centred on , (J2000).

2.2.3 Near-infrared data: VLT and HST imaging

Deep near-infrared () imaging of almost all of the HST ACS field illustrated in Fig. 1 has now been completed with the ISAAC camera on the VLT (Retzlaff et al. 2010). This imaging covers , of which overlaps with the HST ACS imaging. All but 2 of the BLAST sources under study here lie within the area covered by the ISAAC images.

This near-infrared imaging is of excellent quality, with the FWHM of the PSF having a median value of arcsec (it varies from to arcsec across the field; Bouwens et al. 2008). Partly as a result of this good image quality, the point source sensitivity of this imaging is very deep, reaching 5 detection levels of , and (AB magnitudes).

As described by Bouwens et al. (2008), various HST NICMOS and imaging programs have been undertaken in GOODS-South. However, the coverage offered by this imaging is too patchy to be of much use in the present study, and frustratingly (but not unexpectedly) no BLAST source lies within the 5.8 arcmin ultra-deep NICMOS sub-image of the HUDF undertaken by Thompson et al. (2005). However, BLAST 732 does lie within the new Wide Field Camera 3 (WFC3) , , imaging of the HUDF, which reaches a 5- limiting magnitude (AB) of 29 in all three near-infrared bands (McLure et al. 2010; Oesch et al. 2010; Bouwens et al. 2010).

2.2.4 Mid-infrared: Spitzer imaging

Again as part of GOODS, ultra-deep Spitzer imaging with the Infrared Array Camera (IRAC: Fazio et al. 2004) has been obtained over the whole of the ACS GOODS-South field illustrated in Fig. 1 (proposal ID 194, Dickinson et al., in preparation), in all 4 IRAC channels (3.6, 4.5, 5.6, and 8.0 ). The IRAC 5 detection limits are , , , (AB magnitudes).

The 24  Spitzer MIPS data originally obtained as part of GOODS has been augmented and incorporated within the Spitzer Far-Infrared Deep Extragalactic Legacy (FIDEL)111PI M. Dickinson, see survey (Magnelli et al. 2009), and reach 5- detection limits of .

2.2.5 Sub-mm: LABOCA 870  survey

The full  arcmin ECDFS has recently been mapped at a wavelength of 870  by the LABOCA ECDFS Sub-millimetre Survey (LESS) (Weiss et al. 2009). The 12-m diameter of the APEX telescope (Gusten et al. 2006) delivers a 19.2-arcsec FWHM beam. The LESS image has a uniform depth of (as measured in the map, and hence including confusion noise) and the positions and flux densities of the LABOCA sources have been determined in a similar manner to that described above for the BLAST source extraction (Weiss et al. 2009).

The combined analysis of the BLAST and LABOCA LESS source lists and maps in GOODS-South is the subject of a major study which will be presented elsewhere (Chapin et al. 2010). Here we have confined our attention to checking which of the 20 BLAST 250  sources in Fig. 1 are also present in the LESS 870  catalogue presented by Weiss et al. (2009), and briefly exploring the implications of the detections and non-detections (see Section 6.1).

2.2.6 Spectroscopic redshifts

In recent years the GOODS-South field has been the target of a series of spectroscopic campaigns (Dickinson et al. 2004, Stanway et al. 2004, Strolger et al. 2004, van der Wel et al. 2004 Szokoly et al. 2004, Le Fevre et al. 2004, 2005, Mignoli et al. 2005, Doherty et al. 2005, Roche et al. 2006, Ravikumar et al. 2007, Vanzella et al. 2009, Tayler et al. 2009, Eales et al. 2009). Of particular potential importance for the present study has been the completion of the ESO/GOODS VLT/FORS2 programme in the GOODS-South field (Vanzella et al. 2005, 2006, 2008).

The combined impact of these programs is that over 1000 galaxies in the GOODS-South field shown in Fig. 1 now possess reliable spectroscopic redshifts. As a result, and unsurprisingly, it transpires that all except one of the BLAST galaxy counterparts which we identify below with a low-redshift (i.e. ) galaxy already possesses a known spectroscopic redshift.

However, what is perhaps surprising, especially given the work of Vanzella et al., is that only one of the potential higher-redshift BLAST galaxy counterparts currently has a spectroscopic redshift (BLAST 1293, ; Vanzella et al. 2008). As explored further below, this is primarily a consequence of the fact that the high-redshift BLAST galaxy counterparts are too faint/red for optical redshifts to be determined, even in the VLT/FORS2 campaign. The exploitation of the aforementioned multi-waveband photometry for the production of photometric redshift estimates thus remains important for this and future work on the study of sources selected at far-infrared/sub-millimetre wavelengths.

2.2.7 Photometric redshifts

Several photometric redshift catalogues have now been published for the ECDFS in general and for the central GOODS-South field in particular.

The COMBO 17 project (Wolf et al. 2004, 2008) covers the whole  arcmin area of the ECDFS, and exploits 17-band (5 wide and 12 narrow) optical imaging obtained with the Wide Field Imager (WFI) at the ESO 2.2-m telescope. As explained by Wolf et al. (2004, 2008) these ‘very low resolution spectra’ allow solid () photometric redshifts to be obtained down to a magnitude limit of . While the COMBO 17 catalogue contains estimated redshifts reaching , in practice the depth of the optical imaging, and lack of near-infrared information limits its usefulness to where the optical spectroscopy in GOODS-South is very complete. Consequently, a COMBO 17 redshift was only adopted for one BLAST source (BLAST 257-1, ).

Over the  arcmin ECDFS, photometric redshift catalogues based on the available broad-band optical+near-infrared data have been produced by the MUSYC (Multiwavelength Survey by Yale-Chile) collaboration (e.g. Taylor et al. 2009), and (for 24  sources) by Rowan-Robinson et al. (2008). However, of more importance for the current study are the photometric redshift catalogues assembled for the deep central area by the GOODS-MUSIC project (Grazian et al. 2006), by the alternative analyses of Caputi et al. (2006) and Dunlop, Cirasuolo & McLure (2007), and most recently by Brammer et al. (2008), applying the EAZY algorithm to the FIREWORKS data (Wuyts et al. 2008).

We utilised results from these studies but, as described in Section 4, we also decided to derive new redshift estimates for each of the BLAST source candidate identifications. This was partly necessary simply because not all of the sources feature in existing photo- catalogues. However, it also allowed us to check the impact of deriving photometry through different apertures, and to explore the effect on and of allowing extreme values of extinction (see Dunlop, Cirasuolo & McLure 2007).

ID /arcsec ID (J2000) (J2000) / (1.4)
4 1.5 499 53.146221 27.925692 680 20.0 0.0002
6-1 10.8 72 53.124515 27.740279 1100 40.9 0.004
(6-2 9.5 100 53.124986 27.734862 458 26.4 0.008)
59-1 12.2 423 53.079433 27.870691 91 7.9 0.063
(59-2 13.5 240 53.071577 27.872494 102 12.3 0.065)
66 7.2 290 53.020439 27.779829 126 10.2 0.021
104 10.2 370 53.150748 27.825553 89 8.5 0.050
109 7.6 531 53.074414 27.849717 86 6.6 0.035
158 8.6 987 53.090100 27.939860 38 4.6 0.087
193 7.2 53.053608 27.778025 Opt/IR ID
257 10.4 585 53.075206 27.831523 46 6.2 0.092
318 10.8 361 53.180015 27.920681 92 8.8 0.053
503-1 9.7 132 53.157190 27.833468 170 21.0 0.025
(503-2 7.4 315 53.161745 27.832355 65 9.7 0.044)
552 8.9 932 53.052277 27.718325 33 4.7 0.099
593 6.6 677 53.199965 27.904560 44 5.7 0.054
637-1 5.8 110 53.183594 27.862207 290 23.9 0.006
(637-2 9.6 74 53.184536 27.861512 257 39.9 0.015)
654 4.1 53.136577 27.885657 Opt/IR ID
732-1 13.5 53.181458 27.777472 Opt/IR ID
(732-2 5.4 53.180542 27.779686 Opt/IR ID)
(732-3 9.5 53.182018 27.779537 Opt/IR ID)
830-1 7.1 239 53.055171 27.711515 89 12.4 0.030
(830-2 4.2 1179 53.057837 27.713600 30 4.3 0.043)
861 11.9 570 53.198276 27.747894 59 6.4 0.088
983 12.4 405 53.136761 27.769166 100 8.1 0.059
1293 5.2 211 53.193040 27.890814 91 13.2 0.018
Table 2: Galaxy identifications derived from associations with 1.4 GHz VLA sources (17 objects) or analysis of the optical-infrared photometry of possible candidates (3 sources) within a search radius of 15 arcsec. 6 sources have more than one statistically acceptable galaxy counterpart (given in parenthesis). Note that refers to the sum of the individual values of for only the 17 primary (i.e. lower value) radio identifications.
Figure 2: Left: Cumulative distribution of angular offsets between BLAST 250 and radio positions for the 17 radio identifications, compared with the expected distribution for 18 sources given the typical deboosted S/N of the BLAST detections and the size of the 250  Gaussian beam (i.e.  arcsec). Right: The equivalent plot after moving the radio position to the mean of the radio position of the two alternative IDs for the 4 BLAST sources 6, 59, 503 and 830, which all appear to be potential 2-source blends within the BLAST beam. Moving these 4 sources restores the expected behaviour, showing that the distribution of offsets is as expected.

3 Source Identification

3.1 Radio identifications

There is no doubt that, even with the smallest BLAST beam, (FWHM=36 arcsec at 250 ) identifying secure unambiguous optical/IR galaxy counterparts to the far-infrared sources is a challenge. It is also clearly the case that some (possibly large) subset of the BLAST sources may be the product of the blended far-infrared flux density from two or more galaxies at the same, or differing redshifts.

For some of the brighter BLAST sources identified by Dye et al. (2009) and Ivison et al. (2010), sufficiently bright and rare 24  counterparts exist to allow the unambiguous identification of the BLAST sources with Spitzer mid-infrared sources. However, at the fainter flux densities which are the subject of the present study, the sheer number-density of MIPS sources in the deep Spitzer imaging makes the isolation of statistically significant unambiguous mid-infrared counterparts virtually impossible.

We have therefore focussed here on the search for associations with VLA 1.4 GHz sources which, even at the aforementioned deep flux-density limit of , remain sufficiently rare on the sky () for random associations to be statistically unlikely.

3.1.1 Selection of candidate radio counterparts

We searched for radio-source counterparts within a radius of 15 arcsec of each BLAST 250  source. This choice of search radius is not arbitrary, and can be justified in a number of ways.

First, we note that the anticipated positional uncertainty in a source detected with an (undeboosted) signal:noise ratio, S/N, with a Gaussian beam of FWHM , in the presence of background power-law cumulative number counts of the form is given by (Ivison et al. 2007):

Into this expression we insert the FWHM of the BLAST 250  beam , our modal value of S/N = 4.2, and an assumed faint count power-law index (slightly sub-Euclidean number counts appear appropriate at fainter flux densities, as a double power-law fit transits from to at  mJy; Patanchon et al. 2009). The result is . 15 arcsec is then the 2.5 search radius which is expected to contain % of all genuine radio counterparts (see Ivison et al. 2007). Note here that the number count correction term is applied to effectively deboost the source flux density for Eddington bias, and has the effect of reducing a raw S/N = 4.2 to an effective deboosted S/N = 3.4.

Second, while expanding the search radius further might result in one or two additional radio counterparts, the increased number of ways in which a counterpart can be selected inevitably weakens the statistical security of associations which could still have been found within a smaller search radius (see discussion of probability of mis-identification below). From a series of simulations we have established that, given the depth of the radio data available in this field, the number of statistically secure radio identifications is optimised by adoption of a search radius between 12 and 15 arcsec. Fortunately this number is (just) consistent with the 2 to 2.5  positional uncertainty in the BLAST 250  sources under consideration here. This provides some retrospective justification for our decision to confine our study of the faint sources to the BLAST 250  catalogue. It would not be possible to successfully undertake this type of analysis for sources if the beam was much bigger than 36 arcsec (as is the case, for example, at 500 ).

Third, after determining the most likely galaxy identifications, one can check that the distribution of angular offsets is consistent with that expected given the anticipated positional uncertainty in the BLAST sources. We perform this check below, after careful consideration of the confusing effects of source blending.

Finally, we experimented with scaling the search radius with BLAST source S/N, but did not find that this significantly affected the results. In addition, such refinement of the search radius may place too much confidence in the precise accuracy of the positions of the brighter BLAST sources. This is not to say there is any evidence for serious systematic errors in the BLAST positions. Indeed the positional offset of only 1.5 arcsec to the galaxy counterpart of the brightest BLAST source in the field provides confidence that any additional pointing errors in the BLAST 250  positions are minimal. Rather, this is dangerous because, as discussed below (see also Ivison et al. 2010), many of the brightest sources may consist of blends. In this situation, blind application of equation (1) can result in statistically robust primary and secondary radio identifications being missed because of an inadequate search radius (e.g. for BLAST 6, rigorous application of equation (1) would yield a 2.5 search radius of 3.8 arcsec, and a failure to find either of the two contributing galaxies – see Section 3.1.3).

3.1.2 Calculation of probability of mis-identification

Having chosen a candidate radio identification within our 15 arcsec search radius, we then calculate the probability that such a coincidence could have occurred by chance. Following Downes et al. (1986; see also Dunlop et al. 1989), we calculated the raw Poisson probability that a radio source of the observed 1.4 GHz flux density would be discovered by chance at the measured distance from the nominal BLAST source position. We then correct this a priori probability for the number of ways such a statistical coincidence could have been discovered given the available search parameter space defined by the maximum search radius (15 arcsec), the radio-source number density at the limiting search flux-density (), and the form of the radio source counts over the flux-density range of interest (here we adopt a power-law index of ). For the deep data under study here, this correction is often substantial, typically increasing by a factor of a few. This technique has been applied previously to estimate the robustness of radio identifications for SCUBA sources (e.g. Ivison et al. 2002, 2007), and should yield similar results to the method adopted by Dye et al. (2009) based on Monte Carlo simulations.

The value of thus calculated is the probability that the observed association is the result of chance. We stress that even a very low value of does not prove that the radio source is the BLAST source. Nevertheless, a low value of clearly does imply that the radio source is likely related to the BLAST source in some way. This could be true for several reasons. First, the radio source could be the single true counterpart of the BLAST source. Alternatively it could be one of group of 2 or more galaxies which contribute to the BLAST flux-density peak (of particular relevance here, given the large beam-size). Third, the statistical result could be a consequence of some secondary association (e.g. clustering with the true BLAST sources, or the result of gravitational lensing). Despite these worries over statistical interpretation, we re-emphasize that our search for radio counterparts is not motivated purely by their statistical rarity and good positional accuracy, but also by the physical evidence that dust-enshrouded star-forming galaxies also produce copious quantities of synchrotron emission (resulting in the well-known far-infrared:radio luminosity correlation – e.g. Ivison et al. 2010). A sensible hypothesis, therefore, is that an apparently statistically secure radio counterpart to a BLAST source is at least a significant contributor to the observed 250  emission.

3.1.3 Results

The results of this process are tabulated in Table 2. Radio counterparts were found for 17 of the 20 BLAST sources, with multiple counterparts found for 5 of these 17. Half of the BLAST sources have radio counterparts with , and all 17 radio counterparts have . While it would be nice to insist on a significance threshold of , we here adopt as the best that can be realistically achieved given the large search radius required by the BLAST beam. Reassuringly, a sum of the values for the 17 primary identifications yields only , suggesting that source has been misidentified. At the same time our adopted search radius would lead us to expect to have missed true radio identification at larger radii, so our failure to find a radio counterpart for 3 BLAST sources is not altogether surprising. The technique used to isolate the possible optical counterparts for these 3 remaining BLAST sources (listed in Table 2) is explained below in subsection 3.2 (although we note here the possibility that 1 or 2 of these 250  of these sources could be erroneous – see Section 6).

As a consistency check, in the left-hand panel of Fig. 2, we plot the cumulative distribution of angular offsets between BLAST 250  and radio/optical positions for the 17 primary identifications listed in Table 2, and compare this with the ‘expected’ distribution for the afore-mentioned circular Gaussian with  arcsec (assuming 18 sources in total, to allow for the fact our search radius should only include 95% of identifications). While application of the Kolmogorov-Smirnov (KS) test reveals these distributions to only differ at slightly less than the 2 level, this comparison has clearly not worked as well as for SCUBA sources (Pope et al. 2006; Ivison et al. 2007). Closer inspection of Table 2 reveals that, despite low values of , the positional offsets for some of the brighter BLAST+radio associations are surprisingly large. This point is perhaps best illustrated by comparison of the identifications for the brightest two BLAST sources in our sub-sample. For BLAST 4, the radio identification is completely secure () and, as expected, lies only 1.5 arcsec from the BLAST 250  position (predicted positional uncertainty for this 16- BLAST source). By contrast, the most likely identification for BLAST 6, while still statistically compelling (), lies 11 arcsec from the BLAST 250  position, a 7  deviation in positional offset for a 14  BLAST source.

The key to resolving this apparent discrepancy lies in the fact that BLAST 6 has a second (also statistically compelling) radio identification lying almost equi-distant from the 250  position, in the diametrically opposite direction. It turns out that BLAST 6 consists of an interacting pair of galaxies, whose positions (as marked by their VLA centroids) are separated by 20 arcsec, and which both lie at (see Section 4). Clearly the radio identification procedure adopted here has yielded the correct redshift, but the position of the 250  source has either been distorted by contributions from both galaxies, or arises from dust which lies in the region between the two optical galaxies. Either way, the apparently excessive distance to either alternative radio identification should not be naively interpreted as a failure of the radio identification technique, or as casting doubt on the BLAST positional accuracy. Thus, in the case of multiple identifications, each of which appears statistically secure, a fairer assessment of the identification procedure is provided by comparing the BLAST position with the mean position of the two alternative radio identifications, especially when such identifications straddle the nominal 250  position. This is in fact the case for 4 of the 5 BLAST sources listed in Table 2 which have two alternative radio identifications – BLAST 6, 59, 503 and 830. If, for these 4 sources, we replace the primary identification radio source position with the mean radio position of both alternative radio counterparts, the cumulative distribution of positional offsets changes to that presented in the right-hand panel of Fig. 2. This shows that allowance for the possibility of 250  source blending in just these 4 apparently multiply-identified sources, is sufficient to bring the distribution of angular offsets completely into line with expectation.

This analysis provides increased confidence in the statistical robustness of our identification procedure. However, it does serve to highlight the potential problems of confusion arising from the large size of the BLAST beam. In particular it shows that, even when our identification procedure can lead to an unambiguous redshift, it is unclear what fraction of the 250  emission can be reliably attributed to a given radio identification. To explore this further we attempted to distinguish whether, even for a clear-cut high S/N case such as BLAST 6, we could distinguish whether or not the BLAST source was a single source, or a blend of both galaxies. The result, summarized and discussed in Fig. 3, is that we cannot, even when we are confident that the positions of the potentially blended sources are well known, and separated by more than half the FWHM of the BLAST beam. Thus it is clear that we need to be very cautious in attempting to combine 250  and 1.4 GHz data to determine, for example, the far-infrared:radio flux ratio for individual BLAST sources, despite the fact that for only two sources in the current sample (BLAST 59 and BLAST 503) does the choice between two alternative radio identifications significantly influence the inferred redshift (see Section 4). There are clear lessons here that care will need to be taken in deriving the far-infrared spectral energy distribution of sources uncovered by Herschel, especially at 500  where the beam-size is comparable to that which applies here at 250 .

Finally, in Fig. 4 we plot the radio flux-density distribution of the primary identifications listed in Table 2. This figure demonstrates that most of the radio identifications have and that several have flux densities close to the 30 Jy limit. This is another reason that the existence of 3 radio-unidentified sources in our 20-source sample should not be regarded as surprising. Indeed, Fig. 4 makes the generic point that near-complete radio identification of a -selected galaxy sample requires 1.4 GHz radio data reaching at least the same sensitivity in as is achieved at in mJy.

Figure 3: Results of an attempt to deblend the 250  image of BLAST 6. At the top we show a arcsec HST ACS colour image of the field centred on BLAST 6. The upper 2 grey-scale panels then both show the same region as imaged by BLAST at 250  (with 10  arcsec pixels). The single cross in the upper-left image shows the position of a proposed single source which when convolved with the BLAST beam and fitted to the data yields a best-fit flux density of  mJy. When subtracted from the data this leaves the residual image shown in the lower-left panel. The two crosses in the upper-right image show the proposed positions of two distinct sources (i.e. the positions of the radio sources 6-1 and 6-2) which, when convolved with the BLAST beam and fitted to the data, yield best-fit flux densities of  mJy (lower source, 6-1 in Table 2) and mJy (upper source, 6-2 in Table 2). When subtracted from the data this combined-source model leaves the residual image shown in the lower-right panel. Unfortunately, due to the BLAST beam, even in this rather well-defined test case it is not possible to distinguish whether the single or double source model is a better description of the BLAST data, as the single-source fit yields , and the double-source fit yields (for 400 pixels). Thus, while the redshift of this source is not in doubt, and it is clear that both galaxies are related to the 250  emission, it is not possible to decide whether this emission arises primarly between the two optical galaxies, or is a blend of emission from both nuclei.
Figure 4: The distribution of 1.4 GHz radio flux density, in 20 Jy-wide bins, for the radio-identified sources in the 20-source BLAST 250  GOODS-South sample (excluding the two very bright sources at ). All radio flux densities are as given in Table 2. The dotted line marks the 4 30 Jy limit of our radio candidate search in the VLA data. Given this distribution of flux densities, and expecially the fact that several identifications have flux densities just above the 30 Jy limit, the existence of 3 radio-unidentified sources in our 20-source sample is not surprising. This figure demonstrates that near-complete radio identification of a -selected galaxy sample requires 1.4 GHz radio data reaching at least the same sensitivity in as is achieved at in mJy.

3.2 Optical/infrared galaxy counterparts

For the radio-identified sources, determining the correct optical/near-infrared galaxy counterpart is then relatively straightforward, due to the high accuracy of the VLA positions. Most, but not all, of these galaxies are listed in the GOODS-MUSIC catalogue, and we give GOODS-MUSIC ID numbers for each object in Table 3. For those sources which do not feature in GOODS MUSIC we were able to successfully identify the galaxy counterpart in the -band and IRAC imaging (one source, 593, is completely undetected in the ACS optical imaging, even at ), and then performed our own photometry using the available multi-frequency imaging.

This leaves the 3 radio-unidentified BLAST sources, 193, 654, and 732. We must bear in mind the real possibility that, given the S/N ratio of the source catalogue under study, at least one of these 250  sources may not be real. However, as discussed in more detail in the source notes (see Section 5), 193 appears to be confirmed at 350 , 654 appears to be confirmed by a detection at , and 732 has apparently been detected at 870  by LABOCA. We also checked that modest extension of the radio search radius (to 20 arcsec) would still not have yielded a possible radio counterpart for these sources. Thus it seems more likely that these sources may have radio detections lying just below the current radio image threshold, possibly because they lie within the high-redshift tail of the source population.

We therefore attempted to establish ‘best-bet’ optical/infrared counterparts for these sources by deriving a photometric redshift for every possible galaxy counterpart within the same 15 arcsec search radius used for the radio identifications, and then confining our attention to candidates with . The reason for restricting the potential redshift range to is that all three of these BLAST sources, if real, have 250 /1.4 GHz flux ratios , a value which is not exceeded by any known galaxy spectral energy distribution until . As described in more detail in section 5, this yields unique candidates for 193 and 654, and 3 candidates for 732. The positions and GOODS-MUSIC ID numbers (where available) for these objects are also listed in Tables 2 and 3.

The identifications for these sources must inevitably be regarded as more speculative than most of the radio identifications (indeed we later reject 654 on the basis of no detection at 870 or 24). However, the selected objects provide a plausible galaxy counterpart for each of these sources which is at least consistent with the other available photometric and redshift infomation.

The optical, near-infrared and Spitzer photometric data for all 27 galaxies listed in Tables 2 and 3 are presented in Appendix A.

4 Redshifts

4.1 Spectroscopic redshifts

A search of the latest redshift catalogues resulting from the numerous spectroscopic surveys within GOODS-South (see Section 2.2.6) produced redshifts for 13 of the radio-identified galaxy counterparts listed in Table 2. These redshifts are presented in Table 3, where it can be seen that 8 are for primary counterparts, and 5 are for secondary counterparts. The highest spectroscopic redshift is .

4.2 Photometric redshifts

For 637-2 we adopted the COMBO 17 redshift estimate of , but no other galaxy counterpart lacking a spectroscopic redshift has a robust COMBO 17 redshift. Reference to the GOODS-MUSIC catalogue revealed that this is because the remaining candidates all appear to lie at .

Rather than simply adopting the redshift estimates for the higher redshift galaxies from the existing published catalogues, we chose to re-analyse the photometry of each proposed identification to derive our own values of . We chose to do this for 5 reasons. First, not all of the candidates are listed in the existing catalogues, because they are too faint, and for these we had to extract our own photometry from the imaging data and perform the first estimate of their redshifts. Second, given we are potentially dealing with very dusty galaxies, we wished to explore the effect on of allowing extinction () to range to large values (as previously explored in a different context by Dunlop et al. 2007). Third, we wished to to marginalise over the full parameter space to derive meaningful confidence intervals on the estimated redshifts (errors on individual redshift determinations are frequently not provided in the published catalogues). Fourth, we simply wanted to check the robustness of the published redshift estimates, and explore the effect of extracting the photometry through, for example, apertures of different sizes. Fifth, we wish to derive physical parameters such as galaxy age and stellar mass, to facilitate the further study of the physical properties of the BLAST galaxies.

The SED fitting procedure we applied to derive the photometric redshifts and physical properties of the BLAST galaxy counterparts is based largely on the public package Hyperz (Bolzonella et al. 2000). The observed photometry was fitted with synthetic galaxy templates generated with the stellar population models of Charlot & Bruzual (e.g. Bruzual 2007). We used a variety of star-formation histories: instantaneous burst and exponentially declining star-formation with e-folding times , assuming solar metallicity and a Salpeter initial mass function (IMF). For dust reddening we adopted the prescription from Calzetti et al. (2000) within the range . We also included absorption due to clouds along the line of sight in the intergalactic medium, according to Madau (1995).

Our best estimate of for every source (including those with spectroscopic redshifts) is tabulated in Table 3. For every galaxy which lacks a spectroscopic redshift we show in Fig. 5 the best-fitting spectral energy distribution and a plot of versus redshift marginalised over all other fitted parameters (age, star-formation history, dust extinction, and normalization). The confidence interval in redshift is given below each plot.

As a test of the robustness of our photometric redshifts we compare our values for with the available spectroscopic redshifts in Fig. 6. This only provides a direct test out to , but confirms good agreement and reveals no catastropic outliers. In this same figure we also compare our results for the higher redshift sources with the results in the GOODS-MUSIC catalogue, where such values are available. While the scatter in the comparison is inevitably larger, the results still provide confidence that the values of for the higher redshift sources are also reasonably robust.

In Fig. 7 we provide multi-wavelength postage stamp images of the primary BLAST identifications, ranked by redshift. Similar visual information is provided for the secondary/alternative counterparts in Fig. 8.

The final redshift distribution for the GOODS-South 250  ‘brightest-counterpart’ sample is presented in Fig. 10, and discussed in Section 6.2

4 555 0.038 0.05 4.0
6-1 13855 0.076 0.08 4.0
(6-2 13853 0.076 0.08 4.0)
59-1 4107 2.29
(59-2 3920 1.097 1.11 )
66 10764 1.94
104 7347 0.547 0.56 4.0
109 5261 0.124 0.11 4.0
158 136 1.85
193 30093 1.81 4.0
257 6771 0.69 4.0
318 899 2.09
503-1 6790 1.96 4.0
(503-2 6756 0.241 0.31 4.0)
552 30025 1.68 4.0
637-1 4484 0.279 0.26 4.0
(637-2 4578 0.279 0.27 4.0)
654 2977 2.62 4.0
732-1 2.97
(732-2 30080 2.63 )
(732-3 10787 2.40 )
830-1 15626 0.605 0.54 4.0
(830-2 15382 0.735 0.52 4.0)
861 13175 1.95 4.0
983 11348 0.366 0.41 4.0
1293 2645 1.382 1.37 4.0
Table 3: Spectroscopic and photometric redshifts for the BLAST galaxy identifications (including alternative identifications listed in parenthesis). Only for 2 of the 6 sources with alternative identifications does the choice significantly affect the inferred redshift (59 and 503). Also given is the sub-millimetre flux density () or 3- limit taken from the LABOCA LESS survey of GOODS-South by Weiss et al. (2009). Of the 11 proposed BLAST sources with , LABOCA has detected 6. In contrast, no 870  detections were achieved for any of the BLAST sources identified with galaxies at . As discussed in Section 6, this is largely as expected, and provides an independent sanity check on the basic form of the redshift distribution presented here.

5 Notes on individual sources

The brightest 250  source in the field is unambiguously identified with the brightest optical/near-infrared galaxy in GOODS-South. This is a very low-redshift, edge-on disc galaxy in which the effect of patchy dust obscuration can clearly be seen in the HST ACS colour composite image shown in the first panel of Fig. 7. Comparison with the VLA imaging apparently reveals 5 statistically secure alternative radio counterparts (VLA sources 499, 524, 572, 701, 986, all of which have ), but in fact all of these lie near to the centroid of the optical galaxy, and it is clear that the VLA imaging has fragmented a more extended radio source. We have adopted VLA source 499 as the formal radio ID (position listed in Table 2); this is both the closest candidate and has the smallest value of (and is the same radio ID adopted by Dye et al. 2009). A comparison of the sum of the flux densities of the 5 VLA counterparts ( mJy) with the flux density derived from the lower resolution (16 arsec FWHM) ACTA imaging of the field (ACTA ; Norris et al. 2006) confirms that much of the radio emission from the galaxy may have been resolved out by the VLA imaging. Our own sum of all the flux-density in the VLA map yields , and we adopt this as the best available estimate of 1.4 GHz flux density. This lowers the inferred flux density ratio to from the erroneously high value of implied by the numbers quoted in Dye et al. (2009). Given the angular size of the galaxy, and the lack of deep low-resolution radio imaging with a beam size comparable to BLAST, this ratio is still probably an over-estimate of the true value. The fact that the BLAST position lies only 1.5 arcsec from the centroid of the optical/radio galaxy provides confidence in the BLAST 250  positional accuracy because, at S/N = 16, the rms positional error for a BLAST 250  source is expected to be 1.35 arcsec (see Section 3.1). Thus, at least in this region of the 250  map, any systematic pointing error appears impressively small. The source is also clearly detected at 350  and 500 , although the 500  position lies 15 arcsec distant from the true galaxy centroid. This is not hugely unexpected given the rms positional error of 7.5 arcsec anticipated from a 5.5 detection with the 60-arcsec FWHM 500  BLAST beam, but serves as a reminder of why it is virtually impossible to securely identify BLAST 500  sources which lack 250  counterparts.

The second brightest 250  source in the field is clearly associated with an interacting galaxy pair. Both the 250  and 350  positions appear to lie almost equi-distant between two comparably bright, apparently interacting galaxies at the same redshift (see Fig. 1 and Fig. 3). The result is two statistically significant alternative radio IDs (VLA sources 72 and 100), and we have adopted the southern source (VLA 72) as the chosen ID because it has a marginally smaller value of (the 500  position also favours the southern galaxy). It is this galaxy which is shown in Fig. 7, with the alternative galaxy identification shown in Fig. 8. Because both objects lie at the same redshift, the precise choice obviously does not actually affect our final redshift distribution at all. However, in truth the inferred positional offset of 10.4 arcsec between the radio and 250  positions is unexpectedly large for a 14  BLAST source and a 40 VLA source. Thus as discussed in detail in Section 3.1.3, it is essentially certain that the 250  emission either receives comparable contributions from both galaxies, or in fact does actually arise from a region between the two optical galaxies. Unfortunately, as shown in Fig. 3, the BLAST data do not allow us to distinguish between these two scenarios. As with BLAST 4, the integrated 1.4 GHz flux density of this source (quoted in Table 2 for both galaxies) is much larger than the nominal value derived from the VLA radio catalogue by Dye et al. (2009).

         BLAST 59-1:           BLAST 66:
         BLAST 158:           BLAST 193:
Figure 5: Photometric redshift determination for the 12 galaxy identifications in the 20-source BLAST 250  GOODS-South sub-sample which lack spectroscopic redshifts. For each source the upper plot shows the best galaxy spectral energy distribution fit to the HST optical, ISAAC near-infrared and Spitzer 3.6  and 4.5  photometry. The lower plot shows how varies with redshift, marginalised over galaxy age, star-formation history, and dust reddening (allowing the extinction to range up to ). The BLAST ID number of each source, and its estimated redshift (with error range) are given under each two-panel plot.
         BLAST 318:          BLAST 503-1:
         BLAST 552:           BLAST 593:
Figure 5: continued.
         BLAST 654:          BLAST 732-1:
         BLAST 861:           BLAST 1293:
Figure 5: continued.

BLAST 59: (or )
Stepping down by a factor of two in 250  brightness, the third brightest BLAST source has a flux density of mJy, more typical of what is expected in a field of this size given the source counts (Devlin et al. 2009). However, for this object, selection of the correct identification is extremely difficult. The BLAST centroid lies roughly equidistant between 3 alternative radio counterparts. The statistically preferred radio ID for this source lies to the east of the 250  position, but gains additional support from the 500  position. Statistically, the association seems reasonably secure. The radio source has an optical/infrared counterpart in the GOODS MUSIC catalogue (shown in Fig. 7), but this has no spectroscopic redshift. The GOODS MUSIC estimated redshift is , while our own analysis of the photometry yields as shown in the first panel of Fig. 5. However, given the position of the 250  source it is extremely likely that at least some of the far-infrared flux is contributed by the other radio-identified objects, which are galaxies lying within a known large-scale structure at . We thus also retain (as 59-2) the second most likely radio identification, VLA 240, which is a galaxy at which displays AGN emission, and lies to the southwest of the 250  centroid (Fig. 8). This is the one case in the sample where both alternative radio counterparts also appear to be associated with individual LABOCA sources, strengthening the case that the 250  emission results from the blending of at least these two sources.

This 250  source has clear detections at 350  and 500 , both reassuringly close to the 250  position. The radio identification is robust and unambiguous. The source lies just outside the ISAAC near-infrared imaging, but the ACS and Spitzer IRAC photometry is adequate to yield a unique and well-constrained redshift solution at , as shown in Fig. 5. The high-redshift nature of this source receives support from its detection by LABOCA at 870 . The multi-colour postage stamps in Fig. 7 reveal a faint complex source at optical wavelengths, which is bright and unconfused at 3.6 . This is the third of the three sources in this deep GOODS-South sample which were also identified by Dye et al. (2009), and not surprisingly they deduced the same VLA source as the correct ID. Confusingly however, they list a COMBO17 redshift of which is clearly inconsistent with the photometric redshift constraints derived here. However, upon inspection of the latest COMBO17 catalogue it can be seen that the estimated redshift of this source (COMBO17 35066) is highly uncertain (unsurprisingly so, given that the object is very faint, with ) and that the peak of the redshift probability distribution is listed as , consistent with our value. The redshift listed by Dye et al. (2009) can thus be safely rejected.

BLAST 104:
This 250  source has detections at 350  and 500  which reinforce the BLAST position. The VLA identification is centred on a red galaxy with a spectroscopic redshift of . The closest companion seen in Fig. 7 lies at , but the object ENE of the BLAST position has and lies within 28 kpc of the BLAST source at this redshift (although it has no radio detection, so presumably is contributing less to the far-infrared flux density). The next nearest radio counterpart lies 15.7 arcsec north-east of the BLAST position, and thus just outside our adopted search radius. This object has a spectroscopic redshift .

BLAST 109:
This 250  source is not found in the BLAST catalogues at longer wavelengths, suggesting it lies at only moderate redshift. There are two formally-significant radio counterparts, but one lies close to our search boundary at arcsec. We adopt the closer radio counterpart, with the lower value of as the most likely identification. This ties the BLAST source to a low-redshift, edge-on disc galaxy.

BLAST 158:
Secure 350  and 500  counterparts to the 250  source confirm its position as just off the southern edge of the ISAAC -band mosaic. The radio ID is faint, but unique and reasonably secure. As with source 66, the available ACS optical and Spitzer IRAC photometry are sufficient to provide a reasonably solid estimated redshift for the associated galaxy, at , and the high-redshift nature of this source receives support from its detection by LABOCA at 870 . In Fig. 7 the galaxy looks like an extremely complex faint system at optical wavelengths, but it is bright at IRAC wavelengths.

BLAST 193:
This 250  source has a solid detection at 350 , but has no candidate VLA counterpart within our adopted search radius of 15 arcsec (in fact none within 20 arcsec). We therefore fitted galaxy models to the optical-infrared photometry of all objects in the ISAAC -band image within 15 arcsec of the 250  position. This search produced five potential counterparts. Only one of these lies at , and we found this object to also be extremely red. This transpires to be one of only 6 ultra-obscured -selected galaxies in GOODS-South studied in detail by Dunlop et al. (2007; object 1865), and lies only 7 arcsec from the far-infrared position.

BLAST 257:
This 250  source is not found in the BLAST catalogues at longer wavelengths, suggesting it lies at only moderate redshift. This is the second source in the sample which has two alternative radio identifications associated with galaxies at the same redshift. The preferred VLA counterpart (585) has a COMBO17 redshift , while the alternative radio identification (VLA source 852, 19 arcsec distant (so outside our formal search radius) lies in a galaxy with . It seems likely that both galaxies contribute to the 250  flux density, but the precise choice of ID does not affect the final redshift distribution. We adopt the galaxy associated with VLA source 585 as the statistically most likely association.

BLAST 318:
This 250  source has clear detections at 350  and 500 , both reassuringly close to the 250  position. The radio identification is robust and unambiguous, and associated with an interacting galaxy pair (Fig. 7) which the photometry constrains to lie at (Fig. 5). The high-redshift nature of this source gains support from its detection at 870  by LABOCA. VLT FORS2 spectroscopy has been attempted for this object, but yielded no redshift.

Figure 6: A test of the robustness of the new optical-infrared photometric redshifts derived here for the galaxy identifications of the 250  GOODS-South sample. Our new photometric redshifts are compared with the precise spectroscopic values for 8 out of the 9 sources at (solid symbols), and against the published GOODS-MUSIC photometric redshifts for the 8 other sources in the sample for which these are available (open symbols). The former comparison is a true test of the accuracy of our redshift estimates (at least at low redshift), while the latter comparison demonstrates the extent to which independent photometric redshifts agree for the fainter higher-redshift sources in the sample. The agreement is very good, which is perhaps not surprising given the generally well-defined and unique minima in for the individual fits shown in Fig.5.

BLAST 503: (or )
This source is not found in the BLAST catalogues at longer wavelengths, which would suggests it lies at only moderate redshift. However, while there is a possible radio counterpart with a spectroscopic redshift (VLA 315), the statistically preferred option is VLA 132. The optical to infrared images shown in Fig. 7 appear to reveal a complex multiple interacting system, which again is well constrained by the photometry to lie at (Fig.7). The 250  flux density may receive contributions from both sources, but in this case our choice of ID obviously does (strongly) influence the adopted redshift. There is no LABOCA detection to help support a high redshift, but neither does the non-detection strongly exclude it (see Section 6.1).

BLAST 552:
This source may be detected at 350  and 500 , but the positional agreement is poor. We have adopted VLA 932 as the most likely radio identification, but have concerns here about the extent to which the 250  emission in this region is confused by the close proximity of BLAST 830. This is one of the more dubious 250  sources in the sample. For this reason, and because this source does not appear to have been detected at 870  (see Section 6) it has, in the end, been excluded from the final proposed redshift distribution for the sample presented in Fig. 10.

BLAST 593:
This source has no catalogued 350  counterpart, but is a clear detection at 500 , and is nearly coincident with the second brightest LABOCA source in the field. In addition it has a solid and unambiguous radio counterpart in VLA 405. The host galaxy of this radio emission is completely invisible in the optical imaging, perhaps just visible in , but clearly seen at 3.6  (Fig. 7). All evidence points towards a high-redshift dusty galaxy (perhaps the most distant in our sample), but the lack of detections over a wide range in wavelength means that the photometric redshift is poorly constrained (see Fig. 5), and thus we adopt a lower limit for .

BLAST 637:
This 250  source is not found in the BLAST catalogues at longer wavelengths, suggesting it lies at only moderate redshift. There are two alternative formally-significant radio counterparts, and we select the closer and marginally more significant VLA 110 in favour of VLA 74. Both radio sources are associated with galaxies with a spectroscopic redshift , and Fig. 7 indicates that this is another interacting galaxy pair. However, unlike the situation for BLAST 6, the far-infrared position does not lie between the two objects, and favours association with the more luminous galaxy. Clearly the choice of galaxy counterpart does not influence the adopted redshift.

BLAST 654:
This source has no catalogued 350  source, but is detected at 500  only  arcsec distant from the 250  position. This 500  detection, combined with the lack of any radio detection (no counterparts within 30 arcsec), suggest the source lies at high redshift. We therefore fitted galaxy models to the optical-infrared photometry of all objects in the ISAAC -band image within 15 arcsec of the 250  position. This search produced seven potential counterparts. Only one of these lies at , and it is the second closest to the 250  position (4.1 arcsec). It is also favoured by the 500  position. We have therefore adopted this galaxy (GOODS MUSIC 2977, at ) as the best candidate identification in the available data. The GOODS-MUSIC redshift for this galaxy is , in excellent agreement with our own results. The COMBO 17 redshift is , revealing the severe limitations of the COMBO 17 catalogue at faint magnitudes (). As described in Section 6, however, this source does not have a catalogued LABOCA 870 counterpart (as might be expect at high redshift), and it is the only primary BLAST ID with no flux at 24. For these reasons, while we present the information we have gathered on this potential galaxy counterpart, we exclude it from the final redshift distribution for the sample.

BLAST 732: (or )
This source does not have a counterpart at 350  or 500 , but the 250  flux-density is too faint for this to offer a useful redshift constraint. However, the lack of any radio detection suggests the source, if real, lies at high redshift, and indeed the 250  position lies only  arcsec from the fourth brightest 870  LABOCA source in GOODS-South (Weiss et al. 2009). We therefore fitted galaxy models to the optical-infrared photometry of all objects in the ISAAC -band within 15 arcsec of the 250  position. This search produced six potential counterparts, three of which have estimated redshifts . Of these 3, only one has a 24  counterpart, so we adopt this as the primary identification. This object, which we designate 732-1, is a very red galaxy which was too faint to be included in the GOODS-MUSIC catalogue, but which fortuitously lies with the Hubble Ultra Deep Field recently imaged with WFC3 on HST (McLure et al. 2010). The resulting high-accuracy photometry for this source, tabulated in Table A1, yields a very robust photometric redshift , as ilustrated in Fig. 5. The alternative IDs are 732-2, which is GOODS MUSIC 30080 (), and 732-3= GOODS MUSIC 10787 (). Choosing between these alternatives clearly does not significantly affect the final redshift distribution, and it is certainly possible that both the 250 and 870  emission may arise from a blend of a number of sources at .

BLAST 830: (or )
This source does not have a counterpart at 350  or 500 , but the 250  flux density is too faint for this to offer a useful redshift constraint. There are two alternative, statistically-significant radio counterparts, and we select VLA 239 in favour of VLA 1179. The chosen identification appears to be an interacting galaxy with spectroscopic redshift . The edge-on disc galaxy a few arcsec NE lies at and so is not physically associated with the adopted identification. However, the 250  flux density may receive contributions from both these objects, and from VLA 1179. Whatever the exact division of blended emission, it is clear that this 250  arises primarily from sources at .

BLAST 861:
This source does not have a counterpart at 350  or 500 , but the 250  flux-density is too faint for this to offer a useful redshift constraint. The radio indentification, at a radius of 11.9 arcsec, only just passes the adopted significance threshold . This identifies the BLAST source with a faint, red, possibly interacting galaxy, for which the available photometry delivers a unique and well-constrained estimated redshift at . As with BLAST 66, the published COMBO17 photometric redshift is very poorly constrained, and can be safely rejected.

BLAST 983:
This 250  source is not found in the BLAST catalogues at longer wavelengths, suggesting it lies at only moderate redshift. The radio identication is formally secure with . It lies rather far from the 250  position, almost at our limiting search radius, but this is not unreasonable given that it is the second least significant source in our sample. The resulting galaxy identification at can clearly be seen to be dusty in Fig. 7. Only 3 arcsec distant is another less massive red galaxy at essentially the same redshift ().

BLAST 1293:
This source does not have a catalogued counterpart at 350  or 500 , but the 250  flux-density is too faint for this to offer a useful redshift constraint. There are two alternative, formally-significant, radio counterparts, and we select VLA 211 in preference to VLA 148. While the 250  source could be a blend of both objects, our statistically chosen identification transpires to be a bright source at 24 , while the alternative radio counterpart is undetected in the mid-infrared. As can be seen from Fig. 7, our selected identification is a red, high-redshift, apparently interacting galaxy. The GOODS-MUSIC redshift for this object is , but our own photometric redshift for this source is (see last panel of Fig. 5). The latest release of VLT FORS2 GOODS-South redshifts yields (Vanzella et al. 2008).

BLAST 6-1:
BLAST 109:
BLAST 637-1:
Figure 7: Optical/infared postage stamp images of the primary galaxy counterparts we have identified for the 20 BLAST 250  sources in GOODS-South, ranked by redshift (with BLAST source number and redshift given below each left-hand stamp). Each row of stamps commences with a 36 x 36 arcsec HST ACS -band image, centred on the BLAST source position, with the identification search area indicated by the 15 arcsec radius circle. White diamonds mark the available VLA candidate counterparts, with the selected counterpart marked by the orange circle. The remaining three stamps in each row are centred on the position of the selected counterpart, and are 12 x 12 arcsec in size. From left-to-right these show a HST ACS colour image, the -band VLT ISAAC image and the 3.6  Spitzer IRAC image. Display levels on the colour images have been set to for a source, and then these values are reduced by the factor at progressively higher redshifts (to offset surface brightness dimming). In all grey-scale plots black is set to , and white to where is the pixel rms. As explained in Section 2, two sources lie just outside the available near-infrared imaging, and hence lack a -band postage stamp.
BLAST 983:
BLAST 104:
BLAST 830-1:
BLAST 257:
Figure 7: continued
BLAST 1293:
BLAST 552:
BLAST 193:
BLAST 158:
Figure 7: continued
BLAST 861:
BLAST 503-1:
BLAST 318:
Figure 7: continued
BLAST 59-1:
BLAST 654:
BLAST 732-1:
BLAST 593:
Figure 7: continued
BLAST 6-2:
BLAST 503-2:
BLAST 637-2:
BLAST 830-2:
Figure 8: Optical/infrared postage stamp images of the alternative galaxy identifications for 6 of the BLAST sources, including two alternative candidates for BLAST 732. Individual panels are as described in the caption to Fig. 7.
BLAST 59-2:
BLAST 732-2:
BLAST 732-3:
Figure 8: continued

6 Discussion

ID ID /arcsec /arcsec
59 10+34 8.9 7.7 0.004 Blend
66 18 7.5 5.5 0.008
158 79 7.4 5.0 0.011
318 67 12.4 3.7 0.019
593 12 8.7 2.4 0.008
732 32 9.6 4.4 0.012 Opt ID
Table 4: Associations between BLAST 250  and LABOCA LESS 870  sources within the central 150 arcmin of GOODS-South. is the distance, in arcsec, between the BLAST and LABOCA source. For comparison, is the distance, in arcsec, between the LABOCA source and the radio identification listed in Table 2. is the probability that the association between the BLAST and LABOCA source is the result of chance, calculated in an analogous manner to the values calculated for the BLAST-Radio associations in Table 2, but with a search radius of 18 arcsec.

6.1 LABOCA sub-mm detections and 250/870  flux ratios

Within the central area of GOODS-South under study here, Weiss et al. (2009) have extracted 10 LABOCA 870  sources with a raw significance . Searching around the BLAST positions out to a search radius of 18 arcsec, we find that seven of these 870  sources coincide with 250  sources to within a positional accuracy of  arcsec (including two associated with BLAST 59). These associations are tabulated in Table 4. We adopted a search radius of 18 arcsec by adding the positional uncertainty adopted for the BLAST sources in Section 3.1.1 ( arcsec) in quadrature with an assumed positional uncertainty in the LABOCA sources of  arcsec (calculated assuming the 19 arcsec LABOCA beam, and a typical deboosted S/N = 3), and then multiplying by 2.5 to ensure 95% completeness.

The LABOCA and BLAST source surface densities are both so much lower than the radio, mid-infrared or optical source surface densities, that all of these associations are statistically compelling, as demonstrated by the derived values of given in Table 4. The other 3 LABOCA sources in the field are not near to any BLAST source, and so the choice of search radius appears to have been sensible.

Figure 9: The LABOCA LESS 870  detections and non-detections of the BLAST 250  sources. The upper panel shows 870  flux density plotted against redshift (spectroscopic or photometric) as derived from the primary proposed galaxy identification for each BLAST source. All the 870  detections are confined to the high-redshift BLAST subsample. The non-detections are indicated by arrows plotted at the adopted conservative - flux-density limit of . The lower panel plots the derived 250/870  flux-density ratios (or limits), again versus redshift. The anticipated trend of declining 250/870  flux-density ratio with redshift is clearly evident. The solid line, derived by redshifting a simple modified black-body spectrum with  K, and , provides a very good description of the data. The dotted curve shows the effect of increasing temperature to  K, and the dashed line the effect of reducing it to  K. In calculating the observed flux ratios, neither the BLAST nor the LABOCA flux densities have been deboosted.

The associations listed in Table 4 provide an opportunity to check that our adopted positional uncertainties are indeed reasonable. First, the median value of implies that (assuming zero uncertainty in the radio positions), the positional uncertainty in the LABOCA positions is arcsec (allowing for the radial weighting in the observed distribution), showing that our adoption of 4 arcsec was at least approximately correct. The median value of the BLAST-LABOCA positional offset is , implying  arcsec. Subtracting 4.5 in quadrature from 7.5, leads to the conclusion that  arcsec for the BLAST sources, as adopted in Section 3.1.1. Repeating this analysis with means instead of medians, yields  arcsec.

Working backwards, this empirical check on the uncertainty in the positions of the BLAST sources considered in this paper re-affirms that they are indeed genuine sources prior to flux deboosting (including the contribution of confusion to the noise).

The more scientifically interesting aspect of these LABOCA detections is that all of them are associated with high-redshift BLAST sources. The 870  flux densities of the LABOCA detections are listed in Table 3. From examination of this Table it can be seen that the LABOCA detections are confined to proposed identifications with . This point is illustrated in the upper panel of Fig. 9, where we have also adopted a conservative flux-density limit of for the non-detections. Not surprisingly, it can be seen that the redshift distribution of the LABOCA-detected BLAST sources is consistent with that which is displayed by galaxy samples selected at 850 with SCUBA.

The 870 detections thus provide strong, independent support for most of our proposed high-redshift BLAST identifications, especially since the identifications and redshifts were established without any reference to the LABOCA data. However, given the existence of the LABOCA data, one can then also ask whether the LABOCA non-detections of 4 of our proposed identifications cast doubt on their reality. To check this we have therefore plotted, in the lower panel of Fig. 9, the 250/870  flux-ratios of the BLAST galaxies versus redshift. Here, despite the fact that only lower limits are available at low redshift, the anticipated trend of declining 250/870  flux-density ratio with redshift is evident. It is also clear that, with one exception (BLAST 654), the non detection of the high-redshift candidates is not sufficiently deep to cast serious doubt on the proposed redshifts.

The solid curve shown in the lower panel of Fig. 9 is the predicted decline in colour with increasing redshift for a simple modified black-body spectrum with an assumed rest-frame temperature  K and dust emissivity emissivity index . This offers a remarkably good description of the high-redshift data and is at least consistent with the lower redshift limits. In other words, in retrospect we should not be surprised that the 250 -selected galaxies at have not been detected in the LABOCA LESS map, nor that the deep 250  imaging analysed here has reached sufficient depth to allow us to detect the sub-mm galaxy population at . The dashed and dotted curves simply illustrate the effect of increasing or decreasing the assumed dust temperature by 5 K, keeping . Given the mismatch between the BLAST and LABOCA beams, and the fact that neither set of flux densities has been deboosted in constructing Fig. 9, we do not want to over-emphasize the limited extent to which one can determine the temperature of the dust emission from the 250/870  flux-ratios of the BLAST galaxies. However, at the very least, Fig. 9 provides a basic sanity check on the plausibility of our inferred galaxy identifications and redshifts.

6.2 The redshift distribution for the 250  sample

Figure 10: An exploration of the robustness of the basic form of the redshift distribution for the 250  sources in GOODS-South. Sources 654 and 552 have been rejected from both distributions for the reasons detailed in the text. The upper panel shows the redshift distribution derived from the primary identifications (plus 59-2) listed in Table 3. In the lower panel we have replaced the primary identifications by the secondary identifications in the 5 appropriate cases, and in addition have removed the other source which lacks either a radio or a LABOCA counterpart (BLAST 193). Despite these 6 changes, the two distributions are statistically indistinguishable. In the upper panel there are 10/19 galaxies at . In the lower plot there are 8/18 sources at . A median redshift is clearly a fair description of the data presented here, given the uncertainties in identifications and redshifts.

The inferred redshift distribution of our 20-source BLAST 250  sample is presented in Fig. 10. We show two alternative versions, in order to illustrate the extent to which its basic form is robust against changes in ambiguous identifications. BLAST 654 and 552 are excluded from both plots, the former because its 250/870   limit appears anomalously high for its proposed redshift, the latter because its non detection with LABOCA, combined with the low significance of its radio identification and a non detection at 24  casts serious doubt on the robustness of this identification. In the upper panel we plot the histogram derived from the primary galaxy identifications/redshifts listed in Table 3 (we include both 59-1 and 59-2). In this case 10/19 sources lie at , and the distribution appears almost bi-modal. In the lower panel we have replaced the primary identifications with the secondary/alternative galaxy ID for all potentially ambiguous cases (i.e. BLAST sources 6, 257, 503, 732, 830) and have also simply ejected BLAST 193 from the sample (because it possesses neither a VLA radio identification, nor a LABOCA sub-millimetre detection). This more sceptical approach still leaves 8/18 sources at , of which 6 have been detected by LABOCA.

Figure 11: The location of the adopted primary (red circles) and secondary (green stars) galaxy counterparts for the BLAST 250  sources on the Spitzer IRAC colour-colour plane. The small grey points indicate the positions of field galaxies within GOODS-South, as derived from all galaxies in the GOODS-MUSIC catalogue down to limiting IRAC AB magnitudes of . Each BLAST identification is labelled with its redshift. The three tracks are derived by simulating the effect of redshifting, from to , the spectral energy distributions of two well-known local star-forming galaxies (the Virgo Sc galaxy VCC1972, and M82) and the more highly obscured ULIRG Apr220. The blue solid track is for VCC1972, the green dashed track is for M82, and the red dot-dash track is for Arp220, with the SEDs for all three galaxies taken from the multi-wavelength fits derived by Devriendt et al. (1999). The locations of the BLAST primary identifications are in general very well described by the VCC1972 or M82 tracks, which intially move rapidly in observed colour as the 8 PAH feature moves out of the longest IRAC filter, and later move rapidly up in colour as the 1.6 peak in the starlight moves into the filter. Very few of the BLAST galaxies lie on the Arp220/ULIRG track, with the vast majority being far better described by the less reddened star-forming galaxies. At low redshift this tallies well with the appearance of the BLAST identifications shown in Fig. 7, which shows that they are generally isolated dusty star-forming discs. Moreover, certainly at , 250  selection, especially over the relatively small field of GOODS-South will be biased towards cooler SEDs which peak longwards of . This is true for star-forming disc galaxies, but not true for the hotter ULIRGs selected at 60  with IRAS. Perhaps more surprising (given their ‘ULIRG-like’ star-formation rates) is the fact that the BLAST/LABOCA galaxies also appear relatively unobscured at IRAC wavelengths.

For our sample, these two alternative redshift distributions are statistically indistinguishable, and we conclude that, at least in GOODS-South, % of the 250  sources with lie at . Any evidence for bimodality is statistically insignificant, but the median redshift, and the fact that of the sample lies at , appear to be robust results. The precise form of the distribution is of course aflicted here both by small-number statistics, and by the potential effects of cosmic variance. It will therefore be interesting to see the extent to which the redshift distribution derived here applies to the much larger samples of 250  sources which should be uncovered with Herschel.

It is interesting to assess how our results on this small, deep, near-complete BLAST subsample compare with those reported for the full 5- BLAST sample of the wider 9 degree of the Extended Chandra Deep Field South by Dye et al. (2009). This comparison must be done with care, and the limitations understood, because Dye et al. were studying a larger but brighter sample, with on average much poorer supporting data. Dye et al. attempted both radio and 24  identifications for 350 BLAST sources, secured identifications for 198 of them, and in the end secured redshifts for 74 of these (i.e. for 1/5th of the sample). It is not clear what conclusions can be drawn from the resulting redshift distribution, given the low-level of completeness and the mix of flux-density limits.

More instructive for the present comparison is the redshift distribution derived by Dye et al. for the BLAST sources in the central region of the ECDFS, with the best supporting data from the FIDEL survey. Here Dye et al. identified 50% of the BLAST sources (% of the 250 -selected sources) at either radio or mid-infrared wavelengths. The median redshift reported in this sub-area by Dye et al. is . Given that the redshift information includes some COMBO 17 redshifts which (as discussed here for, e.g. BLAST 66) are undoubtedly under-estimates, given that the Dye et al. redshift distribution is more incomplete than that presented here, and given that the effective 250  flux density limit of the Dye et al. deep sample is still % higher than in the present study, we conclude there is no real evidence for any inconsistency between our redshift distribution and that derived by Dye et al. (2009). The only visible difference is that the high-redshift tail in the present deep study extends to somewhat higher redshifts than that reported by Dye et al., but this is unsurprising given the above-mentioned selection effects.

6.3 The mid-infrared colours of the 250  galaxies.

Finally, in Fig. 11 we briefly investigate the location of the galaxy counterparts for the BLAST 250  sources on the Spitzer IRAC colour-colour plane. This is of interest for a number of reasons. First, it is worthwhile to check how the mid-infrared colours of the BLAST-selected galaxies compare with those of the general galaxy population in GOODS-South. Second, we can compare their colours with expectations based on the redshifted SEDs of known local far-infrared bright galaxies. Third, it is of potential interest to check whether the counterparts of 250 -selected galaxies can, in future, be reliably isolated on the basis of IRAC colour (a point of importance given the potentially extensive sky coverage which could be provided by the Spitzer warm mission).

We choose to plot colour versus colour, as advocated by Stern et al. (2005), rather than colour versus colour as advocated by some other authors (e.g. Lacy et al. 2004; Pope et al. 2006). We do this to avoid unhelpful correlations, and because only colours will be available from the Spitzer warm mission.

In Fig. 11 we plot the location of the adopted primary and secondary galaxy counterparts for the BLAST 250  sources, superimposed on the positions of field galaxies within GOODS-South, as derived from all galaxies in the GOODS-MUSIC catalogue down to limiting IRAC AB magnitudes of . In addition, we show tracks in the colour-colour diagram produced by redshifting (from to ) the spectral energy distributions of two well-known local star-forming galaxies (the Virgo Sc galaxy VCC1972, and the starburst galaxy M82), along with the analogous predicted track for the highly-obscured ULIRG Apr 220.

The main points we can learn from this diagram can be summarised as follows. First, the primary BLAST galaxy identifications are very well described by the two star-forming galaxy SEDs, with the red data points essentially mapping out the redshift evolution of the tracks. The rapid horizontal movement at low redshift () is caused by the polycyclic aromatic hydrocarbon (PAH) features moving through the longer two IRAC bands. The subsequent rapid vertical movement from to is the result of the stellar photospheric peak at moving through the shorter two IRAC bands at .

Second, it can be seen that very few of our primary identifications appear to be analogues of Arp 220, although at the very highest redshifts all three templates become indistinguishable. Our low-redshift BLAST galaxies stay relatively blue in colour, indicating their star-light is not swamped by the mid-infrared power-law produced by very hot dust (AGN or starburst heated), as is seen in Arp 220 and other local ULIRGs. Even at most of the BLAST/LABOCA galaxies have colours expected from starlight (albeit in some cases reddened to ). Our highest-redshift candidates do lie in the region of the diagram expected for , but at this point essentially all tracks converge on the same location in the diagram.

It is interesting to speculate why the Arp 220 track is such a poor description of the locus occupied by the BLAST sources. At low redshift it is perhaps unsurprising, as starburst galaxies like M82 and Sc star-forming discs both have (relatively) cool SEDs which peak longward of , whereas the ultra-luminous ULIRGS first uncovered by IRAS at peak at shorter wavelengths. A survey is thus biased towards the selection of these cooler more ‘normal’ starbursts at low redshift, especially since highly-obscured ULIRGs are rather rare objects. The appearance of the low-redshift BLAST galaxies in Fig. 7 (i.e. star-forming discs) is thus consistent with their IRAC colours.

Perhaps more surprising (given their ‘ULIRG-like’ star-formation rates) is the fact that the BLAST/LABOCA galaxies also appear relatively unobscured at IRAC wavelengths. However, this is arguably consistent with their 250/870  flux-ratios as discussed in Section 6.1, which appear to be consistent with a relatively cool dust temperature of 40 K (see Fig. 9).

Finally we revisit the claim made by Yun et al. (2008) that a simple and robust sub-mm galaxy candidate selection criterion is provided by . It is obvious from Fig. 11 that this criterion is in fact satisfied by essentially any galaxy at , and thus cannot be used to isolate any special sub-class of source at these redshifts.

These issues, along with the other physical characteristics of the BLAST galaxies (size, morphology, stellar mass, star-formation history) will be explored in more detail by Targett et al. (in preparation).

7 Summary

We have identified and investigated the nature of the 20 brightest 250  sources detected by BLAST within the central 150 arcmin of the GOODS-South field. Aided by the available deep VLA imaging, reaching (4-), we have identified secure radio counterparts for 17/20 of the 250  sources. The resulting enhanced positional accuracy of arcsec has then allowed us to exploit the deep optical (HST), near-infrared (VLT) and mid-infrared (Spitzer) imaging of GOODS-South to establish secure galaxy counterparts for the 17 radio-identified sources, and plausible galaxy candidates for the 3 radio-unidentified sources.

Confusion is a serious issue for surveys with such large beams, and in many cases there may be no such thing as a unique, single counterpart. We can nevertheless expect our chosen counterparts to be significant, and often dominant contributors to the BLAST flux densities, and we give several arguments to support this claim. It is therefore still reasonable to pursue the properties of this ‘brightest counterpart’ sample. For all of our 20 chosen identifications we have been able to determine spectroscopic (8) or robust photometric (12) redshifts. The result is the first near-complete redshift distribution for a deep 250 -selected galaxy sample. This reveals that 250  surveys reaching detection limits  mJy contain not only low-redshift spirals/LIRGs, but also the extreme dust-enshrouded starburst galaxies previously discovered at longer sub-millimetre wavelengths. Inspection of the LABOCA 870  imaging of the GOODS-South field yields detections of 7 of the proposed BLAST sources, and reveals 250/870  flux ratios consistent with a standard 40K modified black-body fit with a dust emissivity index . Thus, at least in GOODS-South, we infer that % of the 250  sources with lie at .

Based on their IRAC colours, we find that virtually all of the BLAST galaxy identifications appear better described as analogues of the M82 starburst galaxy, or Sc star-forming discs rather than highly obscured ULIRGs. This is perhaps as expected at low-redshift, where the 250  BLAST selection function is biased towards SEDs which peak longward of . However, it also appears largely true at .


JSD acknowledges the support of the Royal Society through a Wolfson Research Merit Award, and the support of the European Research Concil through the award of an Advanced Grant. We acknowledge the support of NASA through grant numbers NAG5-12785, NAG5-13301, and NNGO-6GI11G, the NSF Office of Polar Programs, the Canadian Space Agency, the Natural Sciences and Engineering Research Council (NSERC) of Canada, and the UK Science and Technology Facilities Council (STFC). This work is based in part on observations made with the Spitzer Space Telescope, which is operated by the Jet Propulsion Laboratory, California Institute of Technology under a contract with NASA. APEX is operated by the Max-Planck-Institut fur Radioastronomie, the European Southern Observatory, and the Onsala Space Observatory. This work is based in part on observations made with the NASA/ESA Hubble Space Telescope, obtained from the Data Archive at the Space Telescope Science Institutewhich is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS 5-26555. MC acknowledges the award of a STFC Advanced Fellowship. IRS acknowledges support from STFC. JLW acknowledges the support of an STFC Studentship.


  • [1] Afonso J., et al., 2006, ApJ, 131, 1216
  • [2] Austermann J.E., et al., 2010, MNRAS, 401. 160
  • [3] Beckwith S.V.W., et al., 2006, AJ, 132, 1729
  • [4] Bertoldi F., et al., 2007, ApJS, 172, 132
  • [5] Bouwens R.J., et al., 2008, ApJ, 686, 230
  • [6] Bouwens R.J., et al., 2010, ApJ, 709, L133
  • [7] Bolzonella M., Miralles J.-M., Pelló R., 2000, A&A, 363, 476
  • [8] Brammer G.B., van Dokkum P.G., Coppi P., 2008, ApJ, 686, 1503
  • [9] Bruzual G., 2007, ASPC, 374, 303
  • [10] Calzetti D., et al., 2000, ApJ, 533, 682
  • [11] Caputi K.I., McLure R.J., Dunlop J.S., Cirasuolo M., Schael A.M., 2006, MNRAS, 366, 609
  • [12] Chapin E.L., et al., 2010, MNRAS, submitted (arXiv:1003.2647)
  • [13] Coppin K., et al., 2006, MNRAS, 372, 1621
  • [14] Devlin M.J., et al., 2009, Nature, 458, 737
  • [15] Devriendt J.E.G., Guiderdoni, B., Sadat, R., 1999, A&A, 350, 381
  • [16] Dickinson M., et al., 2004, ApJ, 600, 99
  • [17] Doherty M., et al., 2005, MNRAS, 361, 525
  • [18] Downes A.J.B., Peacock J.A., Savage A., Carrie D.R., 1986, MNRAS, 218, 31
  • [19] Dunlop J.S., Cirasuolo M., McLure R.J., 2007, MNRAS, 376, 1054
  • [20] Dunlop J.S., et al., 1989, MNRAS, 238, 1171
  • [21] Dye S., et al., 2009, ApJ, 703, 285
  • [22] Eales S., et al., 2009, ApJ, 707, 1779
  • [23] Fazio G.G., et al., 2004, ApJS, 154, 10
  • [24] Fixsen D.J., Dwek E E., Mather J.C., Bennett C.L., Shafer R.A., 1998, ApJ, 508, 123
  • [25] Giavalisco, M., et al., 2004, ApJ, 600, L93
  • [26] Grazian A., et al., 2006, A&A, 449, 951
  • [27] Griffin M., et al., 2007, Advances in Space Research, 40, 612
  • [28] Gusten R., et al., 2006, A&A, 454, 13
  • [29] Holland W., et al., 2006, SPIE, 6275, 45
  • [30] Hughes D.H., et al., 1998, Nature, 394, 241
  • [31] Ibar E., Ivison R.J., Biggs A.D., Lal D.V., Best P.N., Green D.A., 2009, MNRAS, 397, 281
  • [32] Ivison R.J., et al., 2002, MNRAS, 337, 1
  • [33] Ivison R.J., et al., 2007, MNRAS, 380, 199
  • [34] Ivison R.J., et al., 2010, MNRAS, 402, 245
  • [35] Kellermann K., et al., 2008, ApJS, 179, 71
  • [36] Lacy M., et al., 2004, ApJS, 154, 166
  • [37] Le Fevre O., et al., 2004, A&A, 428, 1043
  • [38] Le Fevre O., et al., 2005, A&A, 439, 845
  • [39] Madau P., 1995, ApJ, 441, 18
  • [40] Magnelli B., et al., 2009, A&A, 496, 57
  • [41] Marsden G., et al., 2009, ApJ, 707, 1729
  • [42] McLure R.J., Dunlop J.S., Cirasuolo M., Koekemoer A.M., Sabbi E., Stark D.P., Targett T., Ellis R.S., 2010, MNRAS, 403, 960
  • [43] Mignoli M., et al., 2005, A&A, 437, 883
  • [44] Miller N.A., et al., 2008, ApJS, 179, 71
  • [45] Norris R.P., et al., 2006, AJ, 132, 2409
  • [46] Oesch P.A., et al., 2010, ApJ, 709, L21
  • [47] Pascale E., et al., 2008, ApJ, 681, 400
  • [48] Pascale E., et al., 2009, ApJ, 707, 1740
  • [49] Patanchon G., et al., 2009, ApJ, 707, 1750
  • [50] Peacock J.A., et al., MNRAS, 2000, 318, 535
  • [51] Pope A., et al., 2006, MNRAS, 370, 1185
  • [52] Puget J.-L., Abergel A., Bernard J.-P., Boulanger F., Burton W.B., Desert F.-X., Hartmann D., 1999, A&A, 308, L5
  • [53] Ravikumar C.D., et al., 2007, A&A, 465, 1099
  • [54] Retzlaff J., et al., 2010, A&A, 511, 50
  • [55] Roche N.D., Dunlop, J.S., Caputi K.I., McLure R.J., Willott C.J., Crampton D., 2006, MNRAS, 370, 74
  • [56] Rowan-Robinson M., et al., 2008, MNRAS, 386, 697
  • [57] Scott K.S., et al., 2010, MNRAS, 405, 2260
  • [58] Scott S., et al., 2002, MNRAS, 331, 817
  • [59] Serjeant S., et al. 2003, MNRAS, 344, 887
  • [60] Stanway E.R., et al., 2004, ApJ, 607, 704
  • [61] Stern D., et al., 2005, ApJ, 631, 163
  • [62] Strolger L.-G., et al., 2004, ApJ, 613, 200
  • [63] Szokoly G.P., et al., 2004, ApJS, 155, 271
  • [64] Taylor E.N., et al., 2009, ApJS, 183, 295
  • [65] Thompson R.I., et al., 2005, AJ, 130, 1
  • [66] Truch M.D.P., et al., 2009, ApJ, 707, 1723
  • [67] van der Wel A., et al., 2004, ApJ, 601, 5
  • [68] Vanzella E., et al., 2005, A&A, 434, 53
  • [69] Vanzella E., et al., 2006, A&A, 454, 423
  • [70] Vanzella E., et al., 2008, A&A, 478, 83
  • [71] Vanzella E., et al., 2009, ApJ, 695, 1163
  • [72] Viero M., et al., 2009, ApJ, 707, 1766
  • [73] Weiss A., et al., 2009, ApJ, 707, 1201
  • [74] Wolf C., et al., 2004, A&A, 421, 913.
  • [75] Wolf C., Hildebrandt H., Taylor E.N., Meisenheimer K., 2008, A&A, 492, 933
  • [76] Wuyts S., et al., 2008, ApJ, 682, 985
  • [77] Yun M.S., et al., 2008, MNRAS, 389, 333

Appendix A Optical-infrared photometry

Table A1 provides the optical–infrared photometry which was used to derive the BLAST galaxy photometric redshifts.

ID (J2000) (J2000)
4 53.146168 -27.925831 17.590.01 16.570.01 15.970.01 15.620.01 15.110.01 14.830.01 15.410.01 15.880.01 15.380.01 14.110.01 7090709
6-1 53.124493 -27.740086 17.570.01 16.860.01 16.460.01 16.300.01 16.010.01 15.870.01 15.920.01 16.250.01 16.650.01 16.220.01 14.160.01 7590759
109 53.074467 -27.849800 20.360.01 19.100.01 18.410.01 18.070.01 17.480.01 17.110.01 17.000.01 17.430.01 17.750.01 17.830.01 15.950.01 1270127
637-1 53.183559 -27.862030 21.110.01 19.610.01 18.820.01 18.460.01 17.590.01 16.780.01 17.650.01 17.700.01 18.210.01 17.090.01 0594036
983 53.136730 -27.768833 22.490.02 21.100.01 20.390.01 20.030.01 19.410.01 18.860.01 18.300.01 18.870.01 18.770.01 19.130.01 18.020.01 0611010
104 53.150726 -27.825510 22.770.01 21.490.01 20.620.01 20.240.01 19.670.01 19.060.01 18.920.01 19.090.01 19.250.01 19.290.01 19.100.01 0744007
830-1 53.055141 -27.711374 21.830.01 20.920.01 20.060.01 19.840.01 19.250.01 18.630.01 18.800.01 18.990.01 18.870.01 19.130.02 0774010
257 53.075142 -27.831411 23.230.02 21.680.01 20.490.01 20.060.01 19.430.01 18.980.01 18.530.01 18.710.01 19.100.01 19.230.01 19.840.01 0394005
1293 53.193047 -27.890892 26.440.20 26.110.11 25.030.08 24.270.05 22.980.09 21.450.06 20.070.05 20.100.05 20.000.07 20.290.10 0187004
552 53.052277 -27.718325 28.340.54 27.390.21 26.230.14 25.740.11 24.150.09 22.840.06 22.090.08 21.660.11 22.070.92 22.161.09 0290004
193 53.053574 -27.778013 28.130.42 28.700.65 27.180.31 26.270.17 23.980.13 23.290.07 22.580.06 21.530.04 21.320.08 21.250.42 21.950.98
158 53.089821 -27.940001 25.730.09 24.850.05 24.050.04 23.590.04 19.830.04 19.550.04 19.640.07 20.170.13 0586006
66 53.020180 -27.779888 27.730.18 27.130.11 26.560.15 25.430.11 20.840.11 20.350.11 20.210.11 20.830.12 0620007
861 53.198280 -27.747866 27.170.15 26.220.11 25.520.12 24.920.07 23.440.09 22.720.11 22.300.08 20.990.08 20.830.08 20.550.15 20.930.21 0299004
503-1 53.157238 -27.833452 25.900.05 25.260.02 24.550.02 24.180.02 23.150.04 22.460.03 22.130.03 21.070.02 20.730.02 20.800.05 21.210.08 0251005
318 53.179874 -27.920731 25.060.06 24.540.04 24.050.05 23.800.04 22.900.08 21.630.05 20.560.04 20.090.05 19.900.05 20.280.05 0554005