Giant elliptical galaxies are found to have experienced the bulk of their star formation at early times and to have undergone enrichment very rapidly. A similar evolution appears to have taken place in the bulges of spiral galaxies. But how early is "early"? Age dating resolved old stellar field populations in nearby galaxies remains difficult due to crowding, extinction, the superposition of stellar populations of different ages, and the general difficulty of associating individual red giants with a specific age. These problems are exacerbated in galaxies where only integrated-light properties can be analyzed, which makes it very difficult to date stellar populations older than a few Gyr.
An alternative approach, limited to very luminous and hence presumably
very massive, actively star-forming objects, is the analysis of
galaxies observed at high redshift. Surprisingly, even the very young
quasars discovered at a redshift of z ~ 6 (age of the Universe:
~ 900 Myr) reveal metal absorption lines that translate into
supersolar metallicities, indicating very rapid, early enrichment.
These objects may be the precursors of giant ellipticals
(Fan et al. 2001).
The masses of the central black holes in z ~
6 QSOs are estimated to range from several 108 to several
109 M.
This suggests formation redshifts of more than 10 for
putative 100 M
seed black holes if continuous Eddington
accretion is assumed. Other, more rapid black hole formation
mechanisms may also play a role (e.g.,
Fan 2007).
For one of the highest-redshift quasars known,
SDSS J114816.16+525150.3 at z = 6.42,
sub-millimeter and radio observations suggest a molecular gas mass (CO)
of ~ 5 × 1010
M within a
radius of 2.5 kpc around the central black hole if the gas is bound. The
star formation rate in this object is ~ 1000
M
yr-1, akin to what has
been derived for star-bursting ultraluminous infrared galaxies. Even
within 20 kpc, the inferred mass estimate for the QSO's host is still
comparatively low, ~ 1011
M
. A central
massive 1012
M
bulge has
evidently not yet formed
(Walter et al. 2004;
Fan 2007).
In several z
6 QSOs dust has
been detected. One of the
primary sources for dust in the present-day Universe are low- and
intermediate-mass asymptotic giant branch stars, but these need at
least some 500 Myr to 1 Gyr to begin generating dust in their
envelopes. In quasars in the early Universe, other mechanisms are
believed to be responsible, including dust production in supernovae of
type II
(Maiolino et
al. 2004)
and in quasar winds
(Elvis et al. 2002).
Recently two z ~ 6 QSOs
without dust were detected, which indicates that these objects
are probably first-generation QSOs forming in an essentially dust-free
environment
(Jiang et al. 2010).
This discovery illustrates that even at these very early times of less
than 1 Gyr after the Big Bang, galactic environments differ in the onset
of massive star formation and in the degree of heavy-element pollution,
with some regions already having experienced substantial enrichment.
One may speculate that the densest regions are the first ones to start
massive star formation, and that the dusty high-redshift QSOs trace
these regions.
Magnesium, an element,
is produced in supernovae of type II
and hence expected to be generated soon after massive star formation
commences. Iron is predominantly produced in supernovae of type Ia,
requiring a minimum delay time of ~ 300 Myr when instantaneous
starbursts are considered (e.g.,
Matteucci &
Recchi 2001).
Fe is detected in z ~ 6 QSOs despite their
young age. The Fe II / Mg II ratio (which is essentially a
proxy for Fe/
) is found
to be comparable to that of lower-redshift QSOs (e.g.,
Barth et al. 2003;
Freudling et
al. 2003;
Kurk et al. 2007)
and to be around solar or super-solar metallicity. The
near-constancy of the Fe II/Mg II ratio as a function of
redshift implies a lack of chemical evolution in QSOs since z ~ 6
and suggests a formation redshift of the SN Ia progenitors of z
10. Extremely
rapid enrichment on a time scale of just a few
hundred Myr must have occurred in these QSOs, much faster than the
slow enrichment time scales of spiral galaxies. Nonetheless, also
here evolutionary differences are becoming apparent: Some of the z
~ 6 QSOs are less evolved, not showing strong Fe II
emission lines
(Iwamuro et
al. 2004)
and hence no significant SN Ia contributions yet.
Moving to even higher redshifts, the analysis of spectral energy
distributions obtained from near-infrared imaging data of galaxies at
redshifts of 7 (age of the Universe ~ 770 Myr) and 8 (~ 640 Myr)
revealed median ages of ~ 200 Myr for their stellar populations,
but even younger ages are not excluded
(Finkelstein et
al. 2010).
The typical stellar masses of the galaxies at
z ~ 7 are < 109
M; they may be
as low as only 107
M
at z ~
8. While some galaxies are consistent with having no internal dust
extinction, the median value is AV ~ 0.3 mag.
Finkelstein et
al. (2010)
estimate that some 106
M
of dust may
have been produced in these galaxies through massive (12 - 35
M
) stars that
turned into SNe II, a process expected to take less than 20 Myr
(Todini &
Ferrara 2001).
Finkelstein et
al. (2010)
derive metallicities of 0.005
Z for
the majority of their galaxies, while some
may have somewhat higher values (0.02
Z
).
Inferring maximal stellar masses of a few times 109
M
for the
z ~ 7 and 8 galaxies, the authors emphasize that these masses are
still considerably lower than suggested for
L* counterparts at
z < 6. These distant, luminous galaxies whose colors resemble
those of local, metal-poor star-bursting dwarf galaxies trace the earliest
times of high-redshift galaxy formation accessible to us with the
current instrumentation.