  We compute the masses of even spin glueball states $ J^{PC} $, with $ P=C=+1
$, using a twist two operator from an AdS/QCD model known as the hardwall
model, using Dirichlet and Neumann boundary conditions. Within this approach,
we found that the glueball masses are comparable with those in literature. From
these masses, we obtained the Pomeron Regge trajectories for both boundary
conditions in agreement with experimental data available and other holographic
models.
