If dark matter is millicharged or darkly charged, collective plasma processes may dominate
momentum exchange over direct particle collisions. In particular, plasma streaming instabilities
can couple the momentum of the dark matter to counter-streaming baryons or other dark matter and
result in the counter-streaming fluids coming to rest with each other, just as happens for
baryonic collisionless shocks in astrophysical systems. While electrostatic plasma instabilites
(such as the two-stream) are highly suppressed by Landau damping when dark matter is millicharged,
in the cosmological situations of interest, electromagnetic instabilities such as the Weibel can
couple the momenta, assuming that the linear instability saturates in the manner typically found
for baryonic plasmas. We find that the streaming of dark matter in the pre-Recombination universe
is affected more strongly by direct collisions than collective processes, validating previous
constraints. However, when considering unmagnetized instabilities the properties of the Bullet
Cluster merger and other merging cluster systems (which show dark matter streaming through itself)
are likely to be substantially altered if [qχ
/mχ
] ≳ 10-4, where
[qχ
/mχ
] is the charge-to-mass ratio of the dark matter relative to that of the proton.
When a magnetic field is added consistent with cluster observations, the Weibel and Firehose
instabilities result in sufficiently fast growth to reach saturation for [qχ
/mχ
] ≳
10-12–10-11. The Weibel growth rates are even faster in the case of a dark-U(1) charge
(because “hot” electrons do not damp the instability), potentially ruling out [qχ
/mχ
]
≳ 10-14 in the Bullet Cluster system, in agreement with [1]. The
strongest previous limits on millicharged dark matter (mDM) arise from considering the spin-down
of galactic disks [2]. We show that plasma instabilities or tangled background
magnetic fields could lead to diffusive propagation of the dark matter, weakening these spin-down
limits. Thus, plasma instabilities may place some of the most stringent constraints over much of
the millicharged, and our results corroborate previous extremely stringent potential constraints
on the dark-charged parameter space.