4.3. Complications in emission-line analysis
Although the hydrogen and helium lines are basically due to a simple
recombination process, there are various complications in the precise
interpretation of their relative intensities (cf.
Davidson & Kinman 1985)
even when the non-trivial problems of detector linearity, flux
calibration and correction for interstellar reddening have been
overcome. These are the following:
- Unobservable neutral helium in the H+ region. Because He is
abundant enough to soak up its own ionising photons, the degree of
ionisation of trace elements like oxygen or sulphur is not a
straightforwardly good guide to this effect, which is mainly governed
by the effective temperature(s) of the ionising star(s)
(Osterbrock 1974)
and negligible when this exceeds 40,000 K or so.
Vilchez & Pagel
(1988),
following earlier work by
Shields & Searle
(1978)
and Mathis
(1982,
1985),
use a radiation softness parameter
(O+ / O++) / (S+ / S++) as
a measure of the effective temperature and the more recent work avoids
cases where the parameter is so large that the corresponding
ionisation correction factors (icf) read off from photo-ionisation
models
(Mathis 1982;
Stasinska 1982,
1990)
exceed a few per cent and
become model-dependent. Because stellar effective temperatures tend
to be higher in objects with the lowest heavy-element abundances
(e.g.
Campbell 1988),
there is a danger of a spurious dY / dZ
correlation when objects with a large icf are included. Our method
could underestimate the icf in cases where one sees two H II regions
superposed, a hot one with HeI, H I and [O III] and a cooler one with
H I and [O II] but no, or less, HeI
(Pena 1986;
Dinerstein & Shields
1986;
Dufour, Garnett &
Shields 1988),
but in our hottest objects [O
II] is in any case so weak compared to [O III] that this problem
cannot lead to an error as large as 5 per cent
(Pagel & Simonson
1989).
He++ is directly seen by virtue of the
4686 line
in the hottest objects and is easily allowed for.
- Collisional contributions to the emission lines. Because the
23S
state of HeI is highly metastable, it builds up a substantial
population in H II regions and can be excited by electron collisions
to the upper states of the relevant optical lines
(Cox & Daltabuit 1971).
This possibility was generally discounted because of agreement
between triplets and the singlet
6678 in dense planetary
nebulae
(Peimbert &
Torres-Peimbert 1971)
until
Ferland (1986)
drew attention to new quantum-mechanical calculations by
Berrington et al. (1985)
which implied that the singlet states can also be excited from
23S. Ferland deduced some remarkably low helium abundances from
5876
after correcting for the effect; these resulted in part from an
overestimate of the rates by Berrington et al. (since more exact
computation including resonances from enough higher levels is
expensive) but in large part also from a poor selection of data from
the literature on Ferland's part. Anyway, his results were sensational
enough to provoke new, more accurate quantum-mechanical calculations by
Berrington & Kingston
(1987),
giving about half the previous rates, which have been used by
Clegg (1987)
to provide what seem to be
reliable correction formulae depending on electron temperature and
density (which therefore need to be accurately measured).
Peimbert & Torres-Peimbert
(PTP 1987a,
b)
find that, compared to these formulae,
10830
(23Po - 23S) is still anomalously weak
by a factor 2 or so.
Clegg & Harrington
(1989)
consider various effects that could act
to depopulate the 23S state, finding that radiative processes
do not do so appreciably at moderate or low densities. They accordingly
suggest the presence in the planetaries studied by PTP of a hitherto
unknown destruction mechanism (like charge exchange) which would be
inoperative at the low densities of extragalactic H II regions. The
corrections for 4471 and 6678 do not usually exceed a few per cent, in
any case.
- Fluorescence effects. The large population of
23S can also lead to
enhanced production of emission lines by multiple scattering of
ultra-violet photons
(Robbins 1970).
A line especially sensitive to
this is 7065
(33S - 23Po), which is also
relatively strongly
affected by collisional excitation, but can still be used as a test
when this is allowed for. Existing measurements of
7065 (listed by
Pagel 1987a)
show no evidence for significant fluorescence enhancement
of the helium lines from extragalactic H II regions.
- Underlying absorption lines in the stellar continuum. When an H II
region is well resolved, it may be possible to place the slit of the
spectrograph in such a way as to record purely nebular emission, in
which case this problem does not arise. With H II galaxies, however,
which are apparently (and sometimes also intrinsically) very compact,
it is impossible to avoid including the spectrum of the embedded star
cluster with absorption lines of both hydrogen and helium that are
usually unresolved from the nebular emission lines. This problem
particularly affects 4471
and it can be quantified in high
signal:noise spectra by looking for the neighbouring line
4388,
which is comparable or stronger in absorption-line spectra but only
1/7 as strong in emission. Absorption equivalent widths of hydrogen
and helium lines relevant to this problem have been calculated from
evolutionary stellar population synthesis models by
Olofsson (1990).
- Effects of internal dust. While extinction effects of external dust
along the line of sight are readily allowed for by comparison of
observed and theoretical Balmer decrements using a standard reddening
law, internal dust, when present even in small amounts, can cause
substantial complications, e.g. by swallowing up Lyman line photons
and invalidating the standard assumption of Case B recombination. This
problem is quite significant in the case of the Orion Nebula
(Cota & Ferland 1988;
Baldwin et al. 1991)
but probably much less so in
extragalactic H II regions with lower densities and lower abundances.
The effect, if present, must vanish in the limit Z = 0, but it gives
yet another reason for not including Orion in the regression (12) (cf.
Pagel 1982).
- Absorption by intervening gas. Both the Milky Way and the Earth's
atmosphere have absorption lines that can affect HeI
5876 at certain
red-shifts, and a particular problem is presented by Galactic NaI for
objects with red-shifts in the range 0.002 to 0.004 in which many of
the known H II galaxies lie, including both I Zw 18
(Davidson, Kinman &
Freedman 1989)
and II Zw 40 (discussed above). Because of this, and
because of somewhat greater sensitivity to collisional excitation, it
is not advisable to try to deduce a helium abundance from
5876
alone.