LensPerfect Analysis of Abell 1689
The Highest Resolution Mass Map of Galaxy Cluster Substructure To
Date Without Assuming Light Traces Mass
My own release,
including other interesting tidbits
paper: Coe
et al.
2010, ApJ 723,1678 (arXiv)
-- multiple image stamps (17M)
-- delensed multiple image stamps (8M)
Resource paper on dark matter profiles: (Coe 2010, astro-ph/1005.0411)
Comments welcome via e-mail or at
scirate.com (free & easy registration): LPA1689,
DMprofiles

Substructures ~25 kpc across (roughly the visible size of galaxies) on
average are
revealed (contours) within the
central ~400 kpc (diameter) of this galaxy cluster
core, thanks to an analysis of strong gravitational lensing: 135
multiple images of 42 galaxies (and a total of 168 images of 55 knots
within those galaxies) are identified. Their positions (pink squares above; labeled below)
are used to constrain
the distribution of cluster mass (mostly dark matter) interior to them (white outline above).
Multiple images (click to enlarge)

The gravity of A1689 bends the light of more distant galaxies according
to Einstein's General Relativity. We see these galaxies distorted
and displaced, as if through a glass lens. Based on these
displacements, we can determine the strength of this lumpy lens as a
function of position across its surface. It's like a giant
puzzle: We must figure out where all
the mass must be in the core of A1689 to produce the lensed images
where and how we see them.
Our model successfully "de-lenses" the multiple images so we may see
the galaxies as they truly look:
(click to enlarge)

Observed images are in the top row and de-lensed images are in the
bottom row. Note the de-lensed images are all look roughly the
same now,* including clumps oriented the same way, and are at the same
position (see coordinate axes).
*(Note clumps 0,1,2 all align in the delensed images of 10a
&
10b. Clump #10a3 appears to belong to a different galaxy.
And image
#10c has been demagnified, so we don't resolve all the clumps in that
image. Colors in the #10c images appear slightly different as
they
were produced by a different method after modeling and subtracting the
cluster galaxies.)
Our LensPerfect
(Coe08)
mass
model
de-lenses
all
images back to the same "source" position,
down to the individual clumps ...for all 168 images of 55 clumps within
42 lensed galaxies. No other
analysis method can accomplish this. Models of other
methods fail to reproduce the observed multiple image positions by 50
pixels or more. That's ~50x the observational
uncertainties of ~1 pixel. Other methods do well (even perfectly)
by stopping
at ~30 images. However by modeling only ~1/4 the images, they
sacrifice
~4x the mass map resolution (~2x along each axis).

Some of the other methods assume that the visible light traces the
distribution of the mass, including most of the dark matter. We
instead map out the mass (mostly dark matter) without making this
assumption. We can then test how well the light does indeed trace
the mass. Our mass model shows that the light does trace the mass
pretty well, at least qualitatively. However there are some
deviations which we will be
investigating more thoroughly. The mass-to-light ratios of
individual galaxies will also be interesting to measure.
We stress that it can be very useful and informative to assume that
light traces mass. This assumption probably is a good one more
often than not. Ultimately we would like to develop a new method
which assumes that light approximately
traces mass, using the light distribution as a prior on the mass
distribution.
A main scientific result from Coe10 verifies what others have found:
the mass of A1689 is more centrally
concentrated than we expect based on simulations of dark matter
structure formation. (For an explanation, see my DMprofiles
paper.) Some other clusters appear to be similarly
over-concentrated. More definitive results are expected from CLASH, a Multi-Cycle
Hubble Treasury project. If clusters are indeed
over-concentrated, one explanation would be "Early Dark Energy": ~10x
more at early times (e.g., ΩDE ~ 0.10 at z~6) than expected
from ΛCDM (assuming Einstein's
cosmological constant).