Production of dark-matter bound states in the early universe by three-body recombination
A bstract The small-scale structure problems of the universe can be solved by self-interacting dark matter that becomes strongly interacting at low energy. A particularly predictive model for the self-interactions is resonant short-range interactions with an S-wave scattering length that is much lar...
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Veröffentlicht in: | The journal of high energy physics 2018-11, Vol.2018 (11), p.1-33, Article 84 |
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Sprache: | eng |
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Zusammenfassung: | A
bstract
The small-scale structure problems of the universe can be solved by self-interacting dark matter that becomes strongly interacting at low energy. A particularly predictive model for the self-interactions is resonant short-range interactions with an S-wave scattering length that is much larger than the range. The velocity dependence of the cross section in such a model provides an excellent fit to self-interaction cross sections inferred from dark-matter halos of galaxies and clusters of galaxies if the dark-matter mass is about 19 GeV and the scattering length is about 17 fm. Such a model makes definite predictions for the few-body physics of weakly bound clusters of the dark-matter particles. The formation of the two-body bound cluster is a bottleneck for the formation of larger bound clusters. We calculate the production of two-body bound clusters by three-body recombination in the early universe under the assumption that the dark matter particles are identical bosons, which is the most favorable case. If the dark-matter mass is 19 GeV and the scattering length is 17 fm, the fraction of dark matter in the form of two-body bound clusters can increase by as much as 4 orders of magnitude when the dark-matter temperature falls below the binding energy, but its present value remains less than 10
−6
. The present fraction can be increased to as large as 10
−3
by relaxing the constraints from small-scale structure and decreasing the mass of the dark matter particle. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP11(2018)084 |