In total 108 new candidates and 5 known ELGs have been observed. Among them, 81 are new or confirmed emission-line galaxies, 4 are quasars (all with redshifts in the range 3.07 to 3.20), and 8 are galaxies without emission lines. Only 2 of the latter have good enough S/N ratio to identify absorption features enabling measurements of their redshifts. The remaining 20 objects appeared to be either stars with characteristic absorption lines or stellar objects with featureless spectra where the signal-to-noise ratio was insufficient to identify lines.
The new emission line galaxies are listed in Table 2 containing
the following information:
Column 1: The object's IAU-type name with the prefix HS. We note
by asterisk objects observed at Calar Alto.
Column 2: Right ascension for equinox B1950.
Column 3: Declination for equinox B1950.
The coordinates were measured on direct plates of the HQS
and are accurate to
2
(Hagen et al. [1995]).
Column 4: Heliocentric velocity and its rms uncertainty in
km s-1.
Column 5: Apparent B-magnitude obtained by calibration of the digitized
photoplates with photometric standard stars (Engels et al. [1994]),
having an rms accuracy of
for objects fainter than
(Popescu et al. [1996]).
Since the algorithm to calibrate the objective prism spectra is
optimized for point sources the brightnesses of extended galaxies are
underestimated. The resulting systematic uncertainties are expected to
be as large as 2 mag (Popescu et al. [1996]). For about 1/3
of our objects, B-magnitudes are unavailable at the moment. We present
for them blue magnitudes obtained from the APM database. They are
marked by a "plus" before the value in the corresponding
column. According to our estimate they are systematically brighter by
than the B-magnitudes obtained by calibration of the
digitized photoplates (rms
).
Column 6: Absolute B-magnitude, calculated from the apparent
B-magnitude and the heliocentric velocity. No correction for galactic
extinction is made as all objects are located at high
galactic latitudes and because the corrections are significantly smaller
than the uncertainties of the magnitudes.
Column 7: Preliminary spectral classification type according to
the spectral data presented in this article. BCG means that the galaxy
posesses a characteristic H II-region spectrum and that the
luminosity is low enough. SBN and DANS are galaxies of lower
excitation with a corresponding position in line ratio diagrams, as
discussed in Paper I. SBN are the brighter fraction of this type. We
here follow the notation of Salzer et al. (1989). Seyfert galaxies are
separated mainly on diagnostic diagrams as AGN. But if their emission
lines are quite narrow, they probably should be classified as Sy2. SA
is a probable super-association at the rim of an edge-on nearby disc
galaxy. Six objects are difficult to classify. They are coded as
NON.
Column 8: One or more alternative names, according to the
information from NED.
The spectra of all emission-line galaxies are shown in Appendix A, which is available only in the electronic version of the journal.
The results of line flux measurements are given in Table 4.
It contains the following information:
Column 1: The object's IAU-type name with the prefix HS.
By asterisk we note the objects observed during
non-photometric conditions.
Column 2: Observed flux (in
10-16ergs-1cm-2) of the H
line. For the
few objects without an
H
emission line the fluxes are given for H
marked by a
"plus''. For the objects observed on Calar Alto during
non-photometric conditions this parameter is unreliable and marked by
(:).
Columns 3, 4, 5: The observed flux ratios [O II]/H,
[O III]/H
and H
/H
.
Columns 6, 7: The observed flux ratios
[N II]6583 Å/H
,
and
([S II]
6716 Å +
6731 Å)/H
.
Columns 8, 9, 10: Equivalent widths of the lines
[O II]3727 Å, H
and
[O III]
5007 Å.
For the few objects without a detected H
emission line the equivalent
widths are given for H
marked by a "plus''.
Below we give notes on several individual objects:
HS 1015+3717: In the spectrum of this object a cosmic ray hit is
exactly on the line [O III]4959 Å. This was not
corrected in the figure shown in Appendix A.
HS 1214+3801: This is seemingly a supergiant H II-region at
the very rim of the nearby edge-on disc galaxy (SA(s)cd) NGC 4244
(
= 224 kms-1 and
=10.88). At the accepted
distance of NGC 4244 (D = 4.5 Mpc) MB of HS 1214+3801 is about
-
.
The difference between the systemic radial velocity of the
host galaxy and H II-region is small (32 kms-1) and does
not contradict that HS 1214+3801 belongs to NGC 4244. However,
the velocity field of NGC 4244 near the
position of the H II-region is unkown. Both, the single-dish H
I-measurements as summarized in Huchtmeier & Richter
([1989]), and an estimate of the maximum rotational velocity
130 kms-1 (which we obtained through the
Tully-Fisher relation from the absolute B-band magnitude of NGC 4244
of
-
), yield a range of expected velocity differences
between the galaxian material and HS 1214+3801 of up to +160 or
-100 kms-1. But since the 2-D spectrum of HS 1214+3801 with a
total spatial extent of about 20
(
0.5
kpc) shows evidence of internal motions with an amplitude of about
50 kms-1 we need to consider an alternative interpretation for
this object as a companion BCG. Its SF burst may be triggered due to
the tidal effect from the more massive galaxy, similar to the case of
HS 1717+4955 described in Kniazev et al. ([2000]). To
check this option one needs a detailed map of the NGC 4244 velocity field
including HS 1214+3801.
HS 1214+3922: This BCG was reobserved with higher S/N ratio
in order to measure the flux of the [O III]4363 line,
necessary to determine unambiguously the electron temperature
([O III]) of the H II-region and the oxygen abundance.
A preliminary determination according to the procedure described by
Izotov et al. ([1997]) shows that it has
the low oxygen abundance of log(O/H) + 12 = 7.76.
In the course of our follow-up spectroscopy, four QSOs were discovered
with a strong emission line in the wavelength region between 5000 Å and the sensitivity break of the Kodak IIIa-J photoemulsion near
5400 Å. In all of them, we identified Ly1216
redshifted to z
3 as the responsible line. This strong line
produces an easily visible emission peak in the digitized prism
spectra even for very faint objects (B
)
which
is hard to distinguish from low-redshift [O III] features.
Else, QSOs were not selected as candidates for follow-up spectroscopy.
The data for these four new high-redshift quasars are presented in Table 3. Finding charts and plots of their spectra can be found on the www-site of the Hamburg Quasar Survey (http://www.hs.uni-hamburg.de/hqs.html).
In total, for 28 candidates no (trustworthy) emission lines are detected. We divided them into three categories.
For two bright non-ELG galaxies the signal-to-noise ratio of spectra was sufficient to detect absorption lines, allowing the determination of redshifts. The data are presented in Table 5.
To separate the stars among the objects missing detectable emission lines we cross-correlated a list of the most common stellar features with the observed spectra. In total, 13 objects with definite stellar spectra and redshifts close to zero were identified. Four of them are obvious K or M-stars. The rest were classified roughly in categories from definite A-stars to F or G-stars, with most of them intermediate between F and G. The data for these stars are presented in Table 6.
Thirteen non emission-line objects are hard to classify at all. Their
continua have too low signal-to-noise ratio to detect trustworthy
absorption features, or the equivalent width of the emission lines
is too small. Six
of them are certainly non-stellar on DSS images, and classified as
well as non-stellar in the APM database. From our spectra in the range
4000 to
7300-8000 Å, we can exclude the
presence of strong H
.
The remaining 7 objects are
indistinguishable from stellar ones, and we suggest that most of them
are galactic stars. One of the galaxies - namely HS 1232+3609, was
presented after our observations in the paper by Popescu et al.
([1998]) as an ELG with z= 0.2529. Our spectrum is too noisy,
and we could not identify any significant emission with this redshift.
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