-
Articles citing this article
- Same authors
-
Related articles
- Recommend this article
- Download citation
- Alert me when this article is cited
- Alert me when this article is corrected
|
A&A 438, 419-442 (2005)
DOI: 10.1051/0004-6361:20042238
Constraints on Dark Matter interactions from structure formation: damping lengths
C. Boehm1, 2 and R. Schaeffer31 Department of Physics, Theory division, CERN, 1211 Geneva 23, Switzerland
2 LAPTH, 9 chemin de Bellevue, BP 110, 74941 Annecy-Le-Vieux Cedex, France
e-mail: Celine.Boehm@cern.ch
3 SPhT, CEA Saclay, 91191 Gif-sur-Yvette, France
e-mail: Richard.Schaeffer@cea.fr
(Received 22 October 2004 / Accepted 21 February 2005 )
Abstract
Weakly Interacting Massive Particles are often said to be the best Dark Matter candidates. Studies have shown that large Dark Matter-photon or Dark Matter-baryon interactions
could be allowed by cosmology. Here we address the question of the role of the
Dark Matter interactions in more detail to determine at which extent Dark Matter has to be necessarily
weakly interacting. To this
purpose, we compute the collisional damping (and free-streaming) scales of generic interacting Dark Matter
candidates and investigate the effects on structure formation.
Our calculations are valid provided the Dark Matter particles have experienced a phase of
statistical equilibrium at some stage during their evolution.
By comparing these damping lengths to the scale of the smallest
primordial structures known to exist in the Universe, we obtain necessary conditions
that any candidate must satisfy. These conditions are expressed in terms of the Dark Matter
particles' mass and either the total Dark Matter interaction rate or
the interaction rate of Dark Matter with a specific species. The case of Dark Matter interacting with neutrinos or photons is
considered in full detail. Our results are valid even for energy dependent cross-sections and for any
possible initial fluctuations spectrum. We point out the existence of new Dark Matter scenarios
and exhibit new damping regimes.
For example, an interacting candidate may bear a similar damping than that of collisionless Warm Dark Matter particles.
The main difference is due to the Dark Matter coupling to interacting (or even freely-propagating) species. Our approach
yields a general classification of Dark Matter candidates which extends the definitions
of the usual Cold, Warm and Hot Dark Matter scenarios when interactions,
weak or strong, are considered.
Key words: elementary particles -- dark matter -- large-scale structure of Universe
© ESO 2005
| What is OpenURL? |

Document
BibSonomy
CiteUlike
Connotea
Del.icio.us
Digg
Facebook
