A dark matter model where particles and antiparticles have different abundances, preventing annihilation.Asymmetric dark matter is a class of dark matter models in which the abundance of dark matter particles is not balanced by an equal abundance of their antiparticles. In the early universe, if dark matter had symmetric particle-antiparticle populations, they would annihilate each other, leaving only a tiny relic density—far less than the observed dark matter abundance. Asymmetric dark matter avoids this by positing that a particle-antiparticle asymmetry existed from the start, similar to the baryon asymmetry that explains why ordinary matter survived annihilation.
The concept of asymmetric dark matter was developed in the late 2000s, with key papers by Kaplan, Luty, and Zurek (2009) and Nussinov (1985) providing early insights, though the modern framework was solidified in the 2010s.
In these models, a conserved quantum number (analogous to baryon number for ordinary matter) is assigned to dark matter. This asymmetry is generated in the early universe through interactions that violate the symmetry, often linked to the same mechanisms that produce the baryon asymmetry. Once the asymmetry is set, the excess of particles over antiparticles remains, and annihilation processes stop when the minority antiparticles are depleted, leaving the majority particles as the dark matter we observe today. The dark matter mass is then typically in the GeV range, much lighter than the weak-scale masses often considered in symmetric models.
Asymmetric dark matter models are used to predict specific signals in direct detection experiments (like XENON and LUX) and in searches for dark matter annihilation products in cosmic rays, as the annihilation rate is suppressed compared to symmetric models.
In some asymmetric dark matter models, the dark matter particle could be a 'dark baryon' that forms dark atoms, potentially clumping into dark stars or dark disks within galaxies.







