  We compute for the first time the suppression of bottomonia in a strongly
coupled QGP and compare the results to those from a weakly coupled QGP. Using
imaginary time techniques we numerically determine the real and imaginary parts
of the ground state binding energy of the bottomonia in one potential computed
from AdS/CFT and another computed from pQCD. We then use these binding energies
in a suppression model to determine the $\Upsilon$(1S) nuclear modification
factor in $\sqrt{s}_{NN}=2.76$ TeV Pb+Pb collisions. AdS/CFT significantly
overpredicts the suppression compared to data, although the predictive power of
our calculation is limited by its significant sensitivity to the exact details
of the suppression model.
