Existence and multiplicity of $L^2$-Normalized solutions for the periodic Schrödinger system of Hamiltonian type

In this paper, we study the following nonlinear Schrödinger system of Hamiltonian type \begin{equation*} \left{\begin{array}{l} -Δu+V(x)u=\partial_v H(x,u,v)+ωv, \ x \in $\mathbb{R}$^N, \ -Δv+V(x)v=\partial_u H(x,u,v)+ωu,\ x \in $\mathbb{R}$^N, \ \displaystyle\int_{$\mathbb{R}$^N}|z|^2dx=a^2, \end{array}\right. \end{equation*} where the potential function $V(x)$ is periodic, $z:=(u,v):{\mathbb{R}}^N\to \mathbb{R}\times \mathbb{R}$, $\omega \in \mathbb{R}$ appears as a Lagrange multiplier, $a>0$ is a prescribed constant. The existence and multiplicity of $L^2$-normalized solutions for the above Schrödinger system are obtained, and the combination of the Lyapunov-Schmidt reduction, a perturbation argument and the multiplicity theorem of Ljusternik-Schnirelmann is involved in the proof. In addition, a bifurcation result is also given.