SHS spectroscopic follow-up
This is one of the fields imaged in Hα, as part of the AAO UKST Southern Galactic Plane Survey (SHS). This is field 233, centred at 15.4 hrs, -56° (1950) in Norma. It spans a sky area of 4x4 square degrees.
The spectrum obtained per emission line point-source candidate, to date, has sampled the Hα region at a resolution of close to 2 Å (R ˜3000). These data have been gathered mainly using UKST/6dF. Targets were selected for spectroscopy from the imaging survey mainly on the basis of colour-colour diagrams in which apparent Hα 'excess' (obtained on comparing Hα-filter magnitudes with contemporaneous short-red magnitudes to give (R - Hα)) is plotted against broad-band (R - I) colour (the southern I band data also being
available via the ROE SHS database.
To illustrate this approach at work, here are the results from an early
success of the programme -- the discovery of a rare WO star, only the 4th to
be found in the Milky Way. (A full download of the MNRAS paper on
this star, named WR 93b, can be obtained here). At R = 14.7 this object is nearly
5 magnitudes
brighter than the UKST Hα survey limit -- suggesting a lot of room for
many more exciting discoveries.
First, below, a colour-colour diagram for a circular area of sky centred
on the new WO star, 15 arcmin in diameter. Two objects stand out on the
'excess' side of a main locus of stars. The WO star is marked with an arrow.
The other has yet to be followed up spectroscopically.

Figure: (R-Hα) versus (R-I) for point sources with 15 arcmin of
the WO3 star, WR 93b. WR 93b is picked out by the arrow.
Second, the UKST/6dF spectrum obtained using the 1516R grating -- in which
the enormous breadth of the emission line, and its smooth appearance,
immediately point to the object being a Wolf-Rayet star. Furthermore, at the
short wavelength end of the spectrum a weaker emission feature is half picked
up. This is OVI 6200Å, which suggests a refinement of designation to
WO type, which has since been confirmed.

Figure: the discovery UKST/6dF 1516R spectrum of WR 93b
Lastly, below is the optical spectrum from 3700 to 7800 Angstroms made by
combining WHT/ISIS blue-arm and red-arm spectra with a UKST/6dF 580V
observation (bridging the ISIS dichroic gap). Note the enormously bright
CIV 5801,12 Å emission line. This star has turned out to be exceptional
in two respects: it currently holds the record for wind terminal speed
(5750 km/s) among all non-degenerate stars and appears more enriched in carbon
than any other Wolf-Rayet star (C/He = 0.95 by number).

Figure: merged optical spectrum of WR 93b. Relative flux calibration has
been achieved, such that the obviously highly-reddened spectral slope
is reliable.
We have also found a group of 5 WC9 stars in the same part of the Plane as the compact, massive OB association, Westerlund 1. These Wolf-Rayet stars lie within a few degrees with each other on the sky, around Galactic longitude 339, but are not physically associated. The paper describing these is here.
However Wolf-Rayet stars are not common among the emission line objects
being found in this programme. Below are spectra of two less
extreme emission line candidates, with more typical spectra. These were again
obtained using the 1516R grating in UKST/6dF. Note that in both cases the
Hα emission line width is very much narrower than in WR stars, but is
still resolved by the grating.
Figure: 6dF/1516R spectra of a hitherto uncatalogued carbon star (mR = 12.3, black line) and CPD -52° 9243 (mR = 11.3, red
line). The latter has been described as a 'low excitation P Cygni star' by
McGregor et al (1988 ApJ 324 1071). Both are relatively bright objects in field 233, shown at the top of this page.
Our policy has been to aim for data of a quality that will reveal
absorption
line features useful for classification and a broad-brush impression of
distance/luminosity (e.g. the strong diffuse IS band at 6284 Å falls in
the observed range). The spectral resolution
chosen is sufficient to reveal a meaningful intrinsic Hα line profile in
most cases and to provide a measure of FWHM and radial velocity (where the
profile is simple in form). A further advantage of this choice of resolving
power is that it provides a sanity check for any incompletely subtracted
nebular emission -- this will appear as an unresolved emission core superposed
on what, in young and evolved objects, will be broader resolved emission.
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