The optical identification of the first discrete extraterrestrial radio source occurred as a result of a telephone call from J. S. Hey to the Royal Greenwich Observatory on the afternoon of February 28, 1942. Recognizing that the source of extensive jamming of British radar over the previous two days appeared to follow the Sun, Hey was delighted to learn that an unusually large sunspot had just transited the solar disk; despite its skeptical reception by his superiors, Hey's identification proved correct (Hey 1973).
In the ensuing decade, progress in the detection of new extrasolar
radio emitters far outstripped the ability of astronomers to associate
them with optical counterparts. The first breakthrough came in 1949
when Bolton, Stanley and Slee (1949) identified the Crab Nebula, M87,
and NGC 5128 (Cen A) with three of the brightest radio sources in the
sky, although they concluded that the bizarre morphology of the latter
generally favored a Galactic interpretation for radio emitters since
``the probability of [such] an unusual object in our own Galaxy seems
greater than a large accumulation of such objects at a great
distance.'' The following year, Ryle, Smith, and Elsmore (1950)
concurred in this conclusion despite finding 0/146 bright (4.0)
stars, 0/21 novae, 0/38 planetary nebulae, 0/29 diffuse Galactic
nebulae, and 4/5 of the brightest galaxies coincident with entries in
their fifty-source radio catalog. It was not until the classic papers
of Baade & Minkowski (1954a,b), which among other things pronounced
Cygnus A ``an extragalactic affair'', that the era of extragalactic
radio source identification can be said to have begun.
The largest radio catalogs in existence prior to 1995 contained, in
total, approximately 100,000 distinct entries. In striking contrast to
the earliest speculations, fewer than 20 of these relatively bright
radio sources are identified as stars. Indeed, fewer than 1000 stellar
radio detections have been made despite decades of sensitive, targeted
searches (Hjellming 1988 and references therein; Wendker 1995), and
of all cataloged radio sources are Galactic objects. A search of
the NED database, however, suggests that the fraction of identified
extragalactic radio emitters today is little better than it was
in 1950, when 7 out of 67 known radio sources had identified
counterparts (Baade and Minkowski 1954b). The problem now is the same
as it was 50 years ago: the angular resolution of large-area radio
surveys is generally too poor (several arcminutes) to allow for the
unambiguous association of cataloged objects with individual optical
counterparts which, at the limit of the POSS-I plates, number
4000
deg
at high Galactic latitudes. Interferometric surveys at
centimeter wavelengths can achieve the desired positional accuracy of
but have, until recently, covered only
deg
of
sky, resulting in fewer than 500 optical identifications
for radio-selected objects at faint flux levels (see Table 5).
While considerable information on the class and emission mechanism of a
radio source can be derived from observations of its radio morphology, its
spectrum, and its polarization characteristics, optical observations are
still required to establish the source's distance and to classify it
unambiguously. Eight years ago, we began to construct Faint Images of the
Radio Sky at Twenty-cm (FIRST) with the primary goal of obtaining a very
large sample of radio sources with positions sufficiently accurate that
the majority of objects detected could be easily identified on the
basis of positional coincidence alone. FIRST has
been designed to cover the same 10,000 deg region as the Sloan
Digital Sky Survey (SDSS), which will obtain deep optical images of the northern
sky in five colors, and will take spectra of a million objects over the
next decade (Gunn and Knapp 1993). However, an archive of the optical sky
in the form of the National Geographic-Palomar Observatory Sky Survey
(POSS) plates already exists. The identification of even
20% of all FIRST sources with counterparts at or above the POSS
plate limit will immediately provide samples of various radio source
populations from one to three orders of magnitude larger than those in
existence, and will advance significantly our knowledge of the radio
universe.
In this paper, we present the results of an optical identification program for FIRST radio sources based on the Cambridge Automated Plate Measuring Machine (APM) scans of the POSS I plates (McMahon and Irwin 1992). In § 2, we describe briefly the parameters of the FIRST survey and the catalog derived therefrom. In § 3, we describe the genesis of the APM catalog and discuss its astrometric, photometric, and source classification uncertainties with particular attention to those which either 1) the FIRST results can help to refine, or 2) are particularly relevant to radio source identification; the following section (§ 4) demonstrates the utility of FIRST as an astrometric calibrator by deriving both intraplate and plate-to-plate corrections to the optical astrometric solution. Section 5 describes the matching algorithms employed and discusses such issues as false match rates, reliability and completeness of the proposed identifications, and the effects of optical and radio source morphology. Section 6 discusses color, magnitude, and radio flux density distributions for the more than 70,000 counterparts we have identified, while the following section (§ 7) describes the format of the counterpart catalog (the full contents of which are available on the Web). In the discussion (§ 8), we place in context this identification program for faint radio sources, and summarize the statistics of the populations represented. A reprise of our results and a precis of future work concludes our report (§ 9).