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The FLS extragalactic component
D. Ancillary Data

Optical, near-infrared, and radio surveys provide essential support for the extragalactic FLS. The principal requirement is for optical identifications, the first step to understanding FLS sources. Deep (e.g., R ~ 25.5 mag) I- or R-band images covering the full 5 sq.deg. survey area should contain the counterparts of most FLS sources, but we note that accurate (~1 arcsec rms) positions are needed for making reliable optical identifications of such faint infrared objects. The KPNO 4 m telescope is equipped with a large-format camera capable of obtaining such data in a few nights of observing. Most of the detected MIPS sources will have flux densities near the 5*rms detection limit, and their rms positional uncertainties owing to noise alone will be about 10% of the half-intensity beamwidths, or 2 arcsec at 70 microns and 5 arcsec at 160 microns. Such sources may first have to be identified with mid-infrared or radio sources having more accurate positions before being optically identified.

The workshop also recommends covering the extragalactic FLS area with deep (K ~ 18 mag) near-IR images which will be useful for distinguishing stars from galaxies and extending the proposed IRAC spectrophotometry. Again, these data are well within existing capabilities at KPNO, or of an enhanced version of the Two-Micron All-Sky Survey (2MASS) project.

Multicolor (three or more bands) of relatively shallow optical images would be useful for redshift estimates and classification of low-redshift galaxies. The SDSS (Sloan Digital Sky Survey) or the KPNO 0.9 meter telescopes would be capable of obtaining such data.

Radio images are scientifically valuable because most far-infrared sources obey the tight FIR/radio flux correlation. Most radio sources fainter than 1 mJy at 1.4 GHz appear to be powered by starbursts and not AGN, so they probably obey the FIR/radio correlation. Thus deep radio surveys and the extragalactic FLS will find similar source populations, and deep radio surveys can provide pre-launch images that will be similar to the FLS images. The resulting radio catalogs can be used to select and identify most FLS sources for further study before launch. FIR/radio flux ratios can later be used to distinguish objects containing radio-loud AGN from "normal" galaxies. The radio observations should be made with 5 arcsec FWHM resolution (1) to yield sub-arcsec positions for even the faintest detectable sources and (2) to sort out confusion in the larger (20 arcsec at 70 microns, 47 arcsec at 160 microns) MIPS beams.

As a practical matter, only the VLA B-configuration at 1.4 GHz can produce the necessary sky coverage, sensitivity, and resolution. The effective VLA field-of-view is half the beam solid angle, or about 1/7 square deg at 1.4 GHz; thus 35 fields are needed to cover 5 square deg. The 1.4 GHz 5*sigma sensitivies needed to match the FLS shallow survey are listed in the following table:

Radio sensitivities needed to match the shallow FLS
---------------------------------------------------

Wavelength  Sensitivity    1.4 GHz sensitivity
 (microns)    (mJy)              (microJy)

    24         1.3                 90
    70         4.5                 70
   160         27                  80

------------------------------------------------------------------------

These numbers are based on the following assumptions:

  1. In the source frame, (S(60 microns) / S(1.4 GHz)) ~ 140
  2. Radio sources have spectral indices -0.7
  3. Infrared sources have the average spectra of IRAS Bright Galaxy Sample sources
  4. The average redshift of the fainter sources is (z) ~ 1

The VLA can reach the required sensitivity (~15 microJy/beam rms noise) in about 10 hours per field (~350 hours total). In the B configuration, the rms confusion is only about 1 microJy/beam and can be neglected. Fields must be mosaiced in filled hexagonal patterns (seven fields minimum) for uniform sensitivity on the sky, so FLS strips narrower than about 1 deg in either dimension cannot be covered efficiently. Finally, strong sources (1.4 GHz flux densities> several hundred mJy) and low declinations (< +40 deg) must be avoided lest the VLA images be limited by dynamic range, not noise. The VLA will be in the B configuration during the first quarter of 2001.

Go back to Workshop Report or FLS history page.


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This file was last modified on Thu Sep 28 12:46:03 2006.

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