Perfect state transfer in NEPS of complete graphs

Perfect state transfer in graphs is a concept arising from quantum physics and quantum computing. Given a graph $G$ with adjacency matrix $A_G$, the transition matrix of $G$ with respect to $A_G$ is defined as $H_{A_{G}}(t) = exp(-mathrm{i}tA_{G})$, $t in mathbb{R}, mathrm{i}=sqrt{-1}$. We say that perfect state transfer from vertex $u$ to vertex $v$ occurs in $G$ at time $tau$ if $u e v$ and the modulus of the $(u,v)$-entry of $H_{A_G}(tau)$ is equal to $1$. If the moduli of all diagonal entries of $H_{A_G}(tau)$ are equal to $1$ for some $tau$, then $G$ is called periodic with period $tau$. In this paper we give a few sufficient conditions for NEPS of complete graphs to be periodic or exhibit perfect state transfer.