  We test the proposal of arXiv:2012.11274 for the holographic computation of
the charged moments and the resulting symmetry-resolved entanglement entropy in
different excited states, as well as for two entangling intervals. Our
holographic computations are performed in $U(1)$ Chern-Simons-Einstein-Hilbert
gravity, and are confirmed by independent results in a conformal field theory
at large central charge. In particular, we consider two classes of excited
states, corresponding to charged and uncharged conical defects in AdS${}_3$. In
the conformal field theory, these states are generated by the insertion of
charged and uncharged heavy operators. We employ the monodromy method to
calculate the ensuing four-point function between the heavy operators and the
twist fields. For the two-interval case, we derive our results on the AdS and
the conformal field theory side, respectively, from the generating function
method of arXiv:2012.11274, as well as the vertex operator algebra. In all
cases considered, we find equipartition of entanglement between the different
charge sectors. We also clarify an aspect of conformal field theories with a
large central charge and $\mathfrak{u}(1)_k$ Kac-Moody symmetry used in our
calculations, namely the factorization of the Hilbert space into a
gravitational Virasoro sector with large central charge, and a
$\mathfrak{u}(1)_k$ Kac-Moody sector.
