ASTR 333/433 - Dark Matter
Homework 4 - Due at the beginning of class April 23

  1. Cosmic Microwave Background Radiation

    The microwave background consists of relict radiation in a blackbody distribution with
    TCMB = 2.7 K and energy density jCMB = 4 x 10-13 ergs cm-3.

  2. WIMPs in you

  3. WIMP Detection

    WIMP detection experiments are predicated on detecting the kinetic energy deposited by WIMPs scattering off atomic nuclei.
    For elastic scattering, the fraction of the initial kinetic energy Ti transferred from a WIMP of mass mX to a nucleus of mass M is

    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,

  4. Predicting dwarf galaxy velocity dispersions

    Suppose the Milky Way is discovered to have a new dwarf satellite galaxy with the following properties:
    D = 200 kpcRe = 1 kpc M* = 105 M
    A colleague proposes to observe this system to measure its velocity dispersion. Can you predict what she will see?

  5. Donkey Dark Matter

    Professor Mihos once jokingly speculated that the dark matter could be composed of free floating space donkeys (FFSDs).
    Can we constrain this possibility?

    Live Donkeys
    FFSDs would not radiate in the optical, but would emit in the infrared (presuming they have space suits to keep them at a comfortable body temperature of 37 C). If the halo mass of a typical L* (≈ 2 x 1010 L) galaxy is 1012 M, what is its infrared luminosity? How does this compare to its optical luminosity? Could we detect this? (Bear in mind that while IR detector technology lags behind optical detector technology, it has nevertheless gotten pretty good).

    It may help to recall the Wien and Stefan-Boltzmann Laws. To estimate plausible donkey parameters you may assume a spherical donkey.

    ASTR 433 (required); ASTR 333 (extra credit):

    Dead Donkeys
    FFDDs (Free Floating Dead Donkeys - those lacking space suits) would quickly come into thermal equilibrium with the CMB and any other stray energy sources, making them much harder to detect. They would occasionally collide with the Earth.
    Recalling that the collision rate is the product N σ V (number density, cross-section, and relative velocity), compute
    • the approximate frequency of FFDD impacts on the Earth.
    • the kinetic energy deposited by each impact.
    Would we notice this?