Production of dark-matter bound states in the early universe by three-body recombination

被引:28
作者
Braaten, Eric [1 ]
Kang, Daekyoung [2 ,3 ]
Laha, Ranjan [4 ,5 ]
机构
[1] Ohio State Univ, Dept Phys, 174 W 18th Ave, Columbus, OH 43210 USA
[2] Fudan Univ, Key Lab Nucl Phys & Ion Beam Applicat MOE, Shanghai 200433, Peoples R China
[3] Fudan Univ, Inst Modern Phys, Shanghai 200433, Peoples R China
[4] Johannes Gutenberg Univ Mainz, PRISMA Cluster Excellence, D-55099 Mainz, Germany
[5] Johannes Gutenberg Univ Mainz, Mainz Inst Theoret Phys, D-55099 Mainz, Germany
基金
欧洲研究理事会; 美国国家科学基金会;
关键词
Beyond Standard Model; Cosmology of Theories beyond the SM; COSMOLOGICAL SIMULATIONS; SELF-INTERACTIONS; BULLET CLUSTER; ENERGY-LEVELS; SIGNATURES; SYSTEMS;
D O I
10.1007/JHEP11(2018)084
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
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.
引用
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页数:33
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