Hja. Rottgering et al., SPECTROSCOPY OF ULTRA-STEEP SPECTRUM RADIO-SOURCES - A SAMPLE OF Z-GREATER-THAN-2 RADIO GALAXIES, Astronomy and astrophysics, 326(2), 1997, pp. 505-527
We present spectroscopic observations for 64 radio galaxies having ult
ra steep radio spectra. Twenty-nine objects have redshifts z > 2, the
largest redshifts being almost 4. Our ultra steep spectrum (USS) crite
rion (alpha < -1) has proven to be the most efficient way of finding d
istant radio galaxies. We find that even among the USS sources, there
is a strong statistical correlation between the spectral index and red
shift. The most distant radio galaxies within the USS sample have the
steepest radio spectra. In our sample there are 3 radio galaxies at z
> 3 compared with 26 at 2 < z < 3. However, the present data do not al
low us to decide whether there is a decrease in co-moving source densi
ty at the highest redshifts. We have analyzed the spectra of the 30 ob
jects with the highest redshifts (z > 1.9). For these high redshift ra
dio galaxies, Ly alpha is almost always the dominant emission line, wi
th a rest frame equivalent width ranging from similar to 100 Angstrom
to more than 1000 Angstrom. The equivalent widths of the most importan
t emission lines (Ly alpha, C IV, He II, C III]) are found to correlat
e strongly with each other. The large rest frame equivalent widths and
the correlation between the equivalent widths of the emission lines,
confirm that photoionization by a central continuum source is most lik
ely the dominant ionization mechanism. There are significant velocity
differences between the various emission lines of our high redshift ra
dio galaxies; in particular the Ly alpha line is shifted with respect
to the higher ionization lines. Velocity shifts range from 100 to almo
st 1000 km s(-1) in some cases. Simulations show that the effects of a
ssociated H I absorption on the Ly alpha emission line may be responsi
ble for most of these velocity shifts. However, other mechanisms such
as organized kinematics of the Ly alpha emission line gas (e.g. inflow
or outflow) and obscuration of the line emission from the far side of
the radio galaxy may also play a role.