where θ is the scattering angle. A common target nucleus is Xenon, with M = 123 GeV. Assuming that the typical speed of a WIMP in the Milky Way halo is 130 km/s,
Note: Flattened disks rotate faster than the equivalent spherical mass
distribution, leading to one of those geometric factors of order unity.
You may adopt ζ = 0.8, which is a reasonable approximation for
realistic finite thickness disks.
ASTR 433 only: derive and plot the value of ζ
as a function radius for a thin exponential disk by comparing it to the
spherical disk approximation. (Recall Problem 5 of
Homework 1).
Suppose the Milky Way is discovered to have a new dwarf satellite galaxy with the following properties:
D = 200 kpc | Re = 1 kpc | M* = 105 M☉ |
Method 2: Abundance Matching:
Fig. 6 of the review by
Bullock & Boylan-Kolchin
(arXiv:1707.04256)
shows the relation between stellar mass and halo mass
(and Vmax of the halo) obtained from abundance matching.
Use this graph to
Method 3: MOND
The velocity dispersion estimator for an isolated object in the deep MOND regime is
[You can find the value of a0 on the useful numbers page.]
Distinguishing the predictions:
The best observational accuracy that is typically obtained for the velocity dispersion
in such systems is ± 2 km/s.
ASTR 433 only:
Method 4: the External Field Effect
where Gef ≈ (a0/gex)G.
This quasi-Newtonian regime
has a higher effective value for Newton's constant.
A unique feature of MOND is the external field effect (EFE).
When the external field gex of the host exceeds the internal field of
the dwarf satellite, the velocity dispersion estimator becomes
I.e., is gin > gex or gin < gex?
[To estimate gex, assume the rotation curve of the Milky Way
remains flat at 200 km/s.]