5.3. Abundance Results
Table 1 shows the results of applying this analysis
to two bona fide intrinsic absorbers,
namely, the za ze NALs in UM 675
(Hamann 1997;
Hamann et al. 1997b)
and the BALs in PG 1254+047
(Hamann 1998).
The ionic column densities listed for both sources follow from
direct integration of the apparent optical depths in the
absorption line troughs (see Section 5.4 below).
For UM 675, I adjusted the
optical depths for a 50% coverage fraction in all of the metal
ions and 100% coverage in HI. These adjustments do not change
the derived HI column density, but the columns in the metal ions are
roughly doubled. Note
that the relatively low column densities in both systems (and the lack
of a significant HI Lyman edge in UM 675) support the assumption of low
continuum optical depths in the calculations above
(Hamann 1997).
The ionization states in both cases are uncertain, so
the table lists the conservatively low metal-to-hydrogen
ratios, [M/H]p, assuming
each metal line forms at the peak in its f (Mi)
curve. The table also lists the firm lower limits, [M/H]min,
derived from the minimum correction factors in
Hamann (1997).
The uncertainties in the table indicate the range of
values derived for a reasonable range of ionizing continuum shapes.
Keep in mind that these M/H estimates are limiting values that
need not agree between ions.
The [M/H] quantities are typically higher (and more
realistic) for the low-ionization metals because the HI lines
tend to form with these ions. The [M/H]p results provide our
best guess at the actual abundances in UM 675;
the overall metallicity is roughly twice
solar (Z 2
Z
) based on
[C/H], with nitrogen several times more enhanced. The result for Z
Z
is typical of za
ze NALs and occurs without exception in
the intrinsic systems
(Petitjean et al. 1994,
Wampler et al. 1993,
Tripp et al. 1996 and
1997,
Savage & Tripp 1998,
Hamann 1997,
Hamann et al. 1997c).
The NALs thus support the independent evidence
from BELs for Z
Z
and
enhanced nitrogen
(Section 4 above).
![]() |
The derived BAL column densities lead to much more extreme
abundances, with [Si/H]
1.8 and [P/C]
+2.2 in
PG 1254+047. These results are roughly typical of BALs
(Turnshek 1988,
Turnshek et al. 1996,
Korista et al. 1996,
Junkkarinen et
al. 1997,
Hamann 1997).
They are too extreme to be
compatible with well-mixed interstellar gas enriched by normal
stellar populations.
Shields (1996)
noted that the BAL estimates are similar
to the abundances measured in novae. He proposed that novae might
dominate the enrichment of BAL regions if the nova rates are enhanced
by white dwarfs gaining mass as they plunge through the QSO accretion
disk. However, this unusual mechanism is not needed because there
appear to be serious problems with the BAL column densities.