Dark matter that possesses a particle-antiparticle asymmetry and has
thermalised in the early universe, requires a larger annihilation cross-section
compared to symmetric dark matter, in order to deplete the dark antiparticles
and account for the observed dark matter density. The annihilation
cross-section determines the residual symmetric component of dark matter, which
may give rise to annihilation signals during CMB and inside haloes today. We
consider dark matter with long-range interactions, in particular dark matter
coupled to a light vector or scalar force mediator. We compute the couplings
required to attain a final antiparticle-to-particle ratio after the thermal
freeze-out of the annihilation processes in the early universe, and then
estimate the late-time annihilation signals. We show that, due to the
Sommerfeld enhancement, highly asymmetric dark matter with long-range
interactions can have a significant annihilation rate, potentially larger than
symmetric dark matter of the same mass with contact interactions. We discuss
caveats in this estimation, relating to the formation of stable bound states.
Finally, we consider the non-relativistic partial-wave unitarity bound on the
inelastic cross-section, we discuss why it can be realised only by long-range
interactions, and showcase the importance of higher partial waves in this
regime of large inelasticity. We derive upper bounds on the mass of symmetric
and asymmetric thermal-relic dark matter for s-wave and p-wave annihilation,
and exhibit how these bounds strengthen as the dark asymmetry increases.Comment: 31 pages, 8 figures. V2: small corrections, added discussion and
reference