  We apply cluster dynamical mean field theory with an exact-diagonalization
impurity solver to a Hubbard model for magic-angle twisted bilayer graphene,
built on the tight-binding model proposed by Kang and Vafek (2018), which
applies to the magic angle $1.30^\circ$. We find that triplet superconductivity
with $p+ip$ symmetry is stabilized by CDMFT, as well as a subdominant singlet
$d+id$ state. A minimum of the order parameter exists close to quarter-filling
and three-quarter filling, as observed in experiments.
