  We use an energy loss model sensitive to thermal fluctuations to compute the
azimuthal and momentum correlations of $b\bar{b}$ pairs traversing a strongly
coupled plasma from Pb+Pb collisions at LHC ($\sqrt{s}=2.76\text{TeV}$). The
azimuthal correlations are compared with those from perturbative QCD based
simulations. When restricted to leading order production processes, we find
that the strongly coupled correlations of high transverse momentum pairs
($>4\text{GeV}$) are broadened less efficiently than the corresponding weak
coupling based correlations, while low transverse momentum pairs (1-4GeV) are
broadened with similar efficiency, but with an order of magnitude more
particles ending up in this momentum class.
  The strong coupling momentum correlations we compute account for initial
correlations and reveal that the particle pairs suppressed from initially high
momenta to the low momentum domain do not suffice to explain the stark
difference to the weak coupling results in momentum correlations for 1-4GeV.
  From this, we conclude that $b\bar{b}$ pairs are more likely to stay
correlated in momentum when propagating through a strongly coupled plasma than
a weakly coupled one.
