  We investigate the finite-size scaling of the lowest entanglement gap
$\delta\xi$ in the ordered phase of the two-dimensional quantum spherical model
(QSM). The entanglement gap decays as $\delta\xi=\Omega/\sqrt{L\ln(L)}$. This
is in contrast with the purely logarithmic behaviour as
$\delta\xi=\pi^2/\ln(L)$ at the critical point. The faster decay in the ordered
phase reflects the presence of magnetic order. We analytically determine the
constant $\Omega$, which depends on the low-energy part of the model dispersion
and on the geometry of the bipartition. In particular, we are able to compute
the corner contribution to $\Omega$, at least for the case of a square corner.
