Metal Enrichment of the Intergalactic Medium
The paper (700K)
Attachments to the Paper
Color version of
Figure 7
(200x200x15 kpc/h slice) (168K)
Color version of
Figure 8
(200x200x15 kpc/h slice) (202K)
Color version of
Figure 9
(200x200x15 kpc/h slice) (227K)
Color version of
Figure 7a
(200x200x1 kpc/h slice) (191K)
Color version of
Figure 8a
(200x200x1 kpc/h slice) (222K)
Color version of
Figure 9a
(200x200x1 kpc/h slice) (250K)
Explanation
Slices of the gas density (lower row) and the gas temperature
(upper row) of comoving dimensions
200x200x15 kpc/h (as in the paper) and 200x200x1 kpc/h (avaliable only
at this URL)
around the disrupted object at z=11 (Figure 7), z=9 (Figure 8),
and z=7 (Figure 9).
for runs A1 (left column; without
supernovae)
and C1 (right column; with supernovae). Stars are shown
by white symbols. The small square at the center marks the mean cosmic density
for the density panels and T=1000K for the temperature panels.
MPEG video of the process of gas ejection by supernovae:
small format (0.5MB)
large format (1.9MB)
Explanation
Each frame of this video consists of an image like Figures 7-9.
The evolution starts at z=26 (a=0.038) and stops at z=7 (a=0.140).
Note the burst of
star formation in the right panel just before the ejection. Frames
are spaced uniformly in the scale factor with the increment of 0.002.
An
example
of how the merging metal transport mechanism works (163K)
Explanation
You see three rows each showing two slices throughout the whole computational
box: left column shows the gas density, and the right column shows the gas
metallicity. Rows corresponds to z=5.4, z=4.9, and z=4.3 from the top to the
bottom. Stars are shown with while symbols. A zoom into a merger is shown
in the upper right corner of each panel.
There are two separate objects at z=5.4 that are undergoing merger at lower
redshift.
At the
lower row at z=4.3 the dark matter and the star components of the smaller
object passed close to the center of the larger object, while the
gas components of both objects collided in a gigantic shock and merged
at the first impact; as the result the stream of high density gas was
ejected from the merged object (marked with the white circle in the lower row
and pointed to by the arrow). The ejected gas came mostly from
the larger object, and was heavily enriched by metals. In the next
Hubble time or so it will be dispersed and mixed with the
surrounding primeval intergalactic gas, producing high metal abundance
even in low density regions lying close to the merged object. But the
low density gas far from any merger would still be uncontaminated.
My gallery
of computer simulations.