  Recently, Auffinger, Ben Arous, and \v{C}ern\'y initiated the study of
critical points of the Hamiltonian in the spherical pure $p$-spin spin glass
model, and established connections between those and several notions from the
physics literature. Denoting the number of critical values less than $Nu$ by
$\mbox{Crt}_{N}(u)$, they computed the asymptotics of
$\frac{1}{N}\log(\mathbb{E}\mbox{Crt}_{N}(u))$, as $N$, the dimension of the
sphere, goes to $\infty$. We compute the asymptotics of the corresponding
second moment and show that, for $p\geq3$ and sufficiently negative $u$, it
matches the first moment: \[ \mathbb{E}\left\{
\left(\mbox{Crt}_{N}\left(u\right)\right)^{2}\right\}
/\left(\vphantom{\left(\mbox{Crt}_{N}\left(u\right)\right)^{2}}\mathbb{E}\left\{
\mbox{Crt}_{N}\left(u\right)\right\} \right)^{2}\to1. \] As an immediate
consequence we obtain that $\mbox{Crt}_{N}(u)/\mathbb{E}\{ \mbox{Crt}_{N}(u)\}
\to 1$, in $L^2$ and thus in probability. For any $u$ for which
$\mathbb{E}\mbox{Crt}_{N}(u)$ does not tend to $0$ we prove that the moments
match on an exponential scale.
