Annu. Rev. Astron. Astrophys. 1984. 22:
185-222 Copyright © 1984 by Annual Reviews. All rights reserved |
4.2 Three Classes of Models
The models that are reviewed here fall roughly into three classes. In the first type, similar initial conditions are assumed for all galaxies, regardless of their future destiny as cluster or field galaxies. This is the case, for example, in the hierarchical clustering model (Peebles 1974a, b, 1980) with a perturbation spectrum that is nearly white and randomly phased, because in this model the fluctuations that become galaxies reached the nonlinear growth phase long before the cluster-size perturbations. In this sense, galaxies could not ``know'' their future environments. The aim is to reproduce all the morphological variation with fairly late evolution (after clusters became important); for example, S0s might be produced from stripping and ellipticals from merging an initial population of spiral galaxies.
In the second class, later evolution is retained as the primary modifier of galaxy type, in particular through the truncation of disk development, but initial conditions or very early evolution are added to account for the prominence of bulge-dominated galaxies in regions of high galaxy density. This might be accomplished, for example, by dropping the condition of random phasing, so that galaxies with higher central concentration were destined to inhabit regions of high galaxy density (Dressler 1980b), or by including mergers in the early evolution of clusters (the small group phase) to build up a population of more massive spheroids.
If these types of models are unable to explain the morphological data described above (along with the more detailed constraints that will undoubtedly be forthcoming), there is still the possibility that initial conditions were primarily responsible for galaxy morphology. The challenge with this third class of models is to understand how galaxies ``knew'' at the time of their formation about their eventual environments. Recent cosmological models may provide a solution to this problem.
CLASS 1: LATE EVOLUTION
This is not to say that gas ablation is unimportant in the
evolution of spiral galaxies. Although there is still disagreement
over the ease with which gas can be removed from a spiral (cf.
Gisler 1979,
1980,
Kent 1980,
Nulsen 1982),
there is now observational
evidence that such processes could be responsible for the some of the
``anemic'' spirals
(van den Bergh 1976)
in clusters
(Strom & Strom 1979,
Wilkerson 1980,
Sullivan et
al. 1981).
These observations show a
tendency for spirals in the intermediate-density environments (there
are very few spirals in the densest environments) to be gas poor by
factors of 2-3 relative to their field counterparts at the same Hubble
type. These data have been compiled from HI measurements
(Bothun et al. 1982,
Giovanelli et
al. 1981,
and references therein) and from optical
measurements of integrated H flux
(Kennicutt 1983).
Gas depletion,
whether by ablation or exhaustion by star formation (accelerated by
interactions with neighboring galaxies, for example), looks to be a
rather slow process, since the relationships among galaxy gas fraction,
color, and star formation rate are maintained as the gas is removed
(Bothun 1982,
Kennicutt 1983).
Gas ``deficiencies'' of spirals are >modest (factors of 2-3) in
intermediate-density environments, where S0s are quite common. Since
S0s are deficient in gas by factors of 100 or more compared with
spirals, this is further evidence that this type of environmental
influence does not explain the existence of most S0 galaxies. Only in
the Coma cluster has a deficiency of order 10 been
found, and
Bothun (1981)
claims that in this one case there is a population of
small-bulge S0s in the very core, possibly the true remains of
stripped spirals. It is doubtful that a spiral could survive in such
an environment; thus the rarity of small-bulge, gasless systems is
probably a sign that (a) few large D / B spirals have
plunged into these
conditions up to the present-epoch or (b) disk formation is slowest
for these systems, so that their development will be inhibited by the
cluster virialization (see below). On the other hand, ablation may be
very important for gas removal from relatively gas-poor systems like
S0s and ellipticals
(Gisler 1978,
Fabian et al. 1980,
Nulsen 1982).
Toomre & Toomre's
(1972)
suggestion that ellipticals form by
mergers of disk galaxies is another attempt at a class 1 model. This
idea has been more fully developed by
Roos (1981),
who attempts to
build both ellipticals and the bulges of disk galaxies from mergers of
what are initially purely disk systems. The attractions and problems
of such merger models are briefly discussed in the next section.
CLASS 2: LATE EVOLUTION PLUS INITIAL CONDITIONS
Larson et al. (1980;
hereinafter LTC) concentrate their efforts on a
different aspect of the same scheme by suggesting a mechanism for the
``fading.'' Their calculations indicate that gas exhaustion times for
spirals are short, typically a few billion years; therefore, they
suggest that spirals must be refueled by infall from tenuous gas
envelopes. These envelopes would be easily ``stripped'' by tidal
encounters, so a morphology-density relation is expected. This
mechanism should still be effective in lower-density regions (while
those that remove gas directly from the disks are not). Furthermore,
star formation would continue for a few billion years in these
``stripped spirals,'' and this might explain the ``survival'' of blue
galaxies observed by Butcher & Oemler in dense, high-redshift clusters
(see Section 5).
Although gas envelopes of the type required have yet to be observed
(Sancisi 1981,
1983,
and references therein), the
LTC model, like
Kent's, has attractive aspects, and it is the first to make detailed
predictions that can be checked by observations. Like Kent's model,
however, it cannot easily explain the similarity of spiral and S0
LFs. LTC
brushed this problem aside by noting that spheroids in dense
environments appear to be more luminous to begin with (for example,
there are all those ellipticals), so it seems reasonable that the S0s
will come preferentially from large-bulge spirals.
Comparing luminosity functions to test disk truncation and initial
conditions
Schechter's (1976)
analysis of
Oemler's (1974)
data gives
M (Coma)
-M(Hercules) =
0.26, considerably smaller than the value predicted
in the disk-fading model. Indeed, for the average of Oemler's
four ``spiral-rich'' clusters compared with the five ``cD'' clusters
(lowest proportion of spirals), M =
-0.21, which goes in the wrong
sense for the disk-fading model. An even larger value of M ~ 1.2
magnitudes is to be expected in comparing a ``faded field'' population
(<D / B> ~ 5) with the population of the Coma core (<D /
B> ~ 0.8), but,
in fact, there is no significant difference in M for any region of
Coma compared with the field.
If these data are corroborated by better-quality photometric
observations, then the inference will be clear: a brightening of
spheroids by factors of 2-3 in dense regions is needed to compensate
for the lower luminosities of disks and thus leave the LF basically
unchanged. It is perhaps encouraging that early attempts to model
cluster evolution
(Miller 1983,
Malumuth &
Richstone 1984)
do show an approximate balance between the opposing effects of mergers
and tidal stripping.
In summary, it is difficult to account for the data on
morphological types, D / B, and LFs as a function of environment without
appealing to both disk truncation and larger spheroidal components in
dense regions. Since a disk luminosity function for the Coma cluster
would include few luminous systems like those found in the low-density
field, it seems reasonable to conclude that a disk truncation
mechanism is at work. Furthermore, as pointed out by
Ostriker (1977),
the mass of intracluster gas in Coma is roughly what would remain if
disks of the size found in field spirals were prevented from forming.
(This implies, moreover, that the fraction of mass in ``left over'' gas
will be found to be a function of spiral fraction, and that little
residual gas should be found in the field.) By implication, the
spheroidal LF, like the disk LF, must also be different in clusters
than in the field (since the spheroidal + bulge = total LFs are so similar).
Building up spheroids by mergers
Some of the early objections to making ellipticals from basically
stellar mergers (see, for example,
Ostriker 1980)
appear to have weakened. Numerical simulations (e.g.
White 1978,
Farouki et al. 1983)
indicate that central densities can grow as mergers proceed
(nonhomology), and central velocity dispersions may also rise. Both
are necessary if ellipticals are to be produced. A study by
Dressler & Lake
(1984)
of about 15 disturbed systems from the
Arp (1966) and
Arp & Madore (1984)
catalogs of peculiar galaxies confirms that the
central velocity dispersions are in reasonable accord with the
Faber-Jackson relation
(1976)
for ellipticals, i.e. these probable
mergers already match ellipticals in the L- diagram. Schweizer
(1982,
1983)
has presented empirical evidence that mergers of field
galaxies are common and may result in elliptical galaxies. For
example, he claims that the luminosity profile of the highly
interactive NGC 7252 system will eventually match the
R1/4 form of
typical of ellipticals. The shells and plumes around many ellipticals
(Arp 1966,
Malin & Carter 1980)
may be further evidence that ``field
ellipticals'' (those in low-density regions) are in environments that
favor mergers, since such features may result from the infall of disk
galaxies
(Quinn 1983).
The objection that ellipticals are common in rich clusters, where
the high relative velocities suppress mergers, is probably negated by
the likelihood that the merging occurred when the cluster was a
collection of small groups (see, for example,
Geller & Beers 1982)
in which the velocity dispersions were much lower. This could also
explain the existence of field ellipticals as the remnants of mergers
of compact groups of galaxies
(Carnevali et
al. 1981).
(In general,
it is likely that the evolution of the different morphological types
must have begun at a time when the density contrast from the field to
the clusters was much smaller than it is today, since morphology is a
very slow function of local density.)
Nevertheless, serious problems remain for the theory.
Harris (1981)
claims that a difference in globular cluster frequency per unit
luminosity for spirals compared with ellipticals may be evidence
against a merger origin for ellipticals.
Sandage (1983)
points to a
continuity of properties from dwarf ellipticals to luminous systems (a
factor of 104 in luminosity) as an argument against mergers,
since it
is unlikely that the dwarf ellipticals were also made by mergers. The
observational data on color (abundance) gradients are still sparse,
and the extent to which such gradients would be erased by merging is unclear
(White 1980,
Villumsen 1982);
however, the general trend of
redder colors and higher metallicities for brighter systems
(Faber 1973,
Sandage &
Visvanathan 1978)
must certainly be explained.
Are mergers responsible for building the bulges of disk galaxies as
well? Bulges and low-luminosity ellipticals are isotropic rotators;
therefore, they could have developed along the lines of the classical
collapse models
(Eggen et al. 1962,
Larson 1976,
Gott & Thuan 1976).
In this simple picture, mergers are perhaps responsible only
for the ``giants,'' the most massive ellipticals, which are slowly
rotating and have low surface brightnesses. But if mergers are to help
account for all large spheroids in dense regions, then they must
produce some larger-bulge disk galaxies as well. This raises a number
of additional problems, such as explaining why disk systems held on to
some of their gas while the ellipticals did not. If the gas that
formed the disk fell in well after the merger that produced the bulge,
can the angular momenta of disk and bulge be expected to align as well
as they do (see
Gerhard 1981)?
Why are even the most luminous bulges
flattened by rotation
(Kormendy &
Illingworth 1982,
Dressler & Sandage
1983),
while the most luminous ellipticals are not? In the case of our
own Galaxy, it has been proposed that gas lost from a spheroid that
formed prior to the disk explains otherwise puzzling features of the
chemical enrichment history
(Ostriker & Thuan
1975).
Are these data
consistent with a model where disks formed first, and bulges followed
afterward from mergers or accretion? A merger model that can explain
all of these observations, together with a limitation on disk building
as a function of density, can probably account for all basic
properties of the morphological types, and the morphology-density
relation as well.
CLASS 3. INITIAL CONDITIONS
The deficiency in these models that employ only initial conditions is
that they provide no obvious explanation for the observed
dependence of morphology on later environment. To achieve this, the
perturbation that becomes the protogalaxy must be affected by the
larger scale perturbation that grows into a group or cluster. In a
crude sense, they must form at the same time. For a white noise
spectrum, this can be accomplished by abandoning random phasing so
that the largest amplitude galaxy perturbations are always found
within the largest amplitude cluster perturbations. For the
isothermal perturbation model (hierarchical clustering;
Peebles 1974a,
b,
1980),
the same results can be achieved if the initial
spectrum contained more power at large scales (pink noise). The
adiabatic perturbation models
(Doroshkevich et
al. 1980,
and references therein) have a built-in preferred scale of large
mass. These conditions result in earlier growth of the groups and
clusters relative to the galaxies; therefore, the final amplitude of a
protogalaxy fluctuation will depend on whether it is in a protocluster
or protofield region. The recent emphasis on cosmologies with exotic
particles that dominate the mass of the Universe has produced several
models where these preferred mass scales for galaxies and clusters are
expected [see
Primack &
Blumenthal (1983)
for a review], and within
these types of models such coupling of galaxies to clusters is likely,
if not unavoidable. High-energy physics, then, could supply the extra
ingredient that enables the construction of galaxy formation models
that rely primarily on initial conditions.
Alternatively, it has been suggested that differences might arise in
the angular momentum gained through tidal torques
(Peebles 1969)
in protocluster and protofield regions
(DiFazio &
Vagnetti 1979,
Shaya & Tully 1984).
Large-scale variations in the distribution of angular
momentum would provide a correlation with environment for the model of
galaxy differentiation first suggested by
Sandage et
al. (1970).
At present, it might be best to consider these types of models as
``last resorts.'' Our ignorance of initial conditions is greater than
our ignorance of later evolutionary effects ; therefore, such models
are rather ad hoc and offer few predictions or tests. Until they are
able to do so, it seems advisable to embrace this alternative only if
the models that stress later external influences fail to explain the
data on morphological types and their environments.
2 The author has checked this by fading each
galaxy in the Hercules sample individually and finds the expected shift
of M ~ 1.0. Back.