Let $\mathbb{T}^3=(\mathbb{R}/\mathbb{Z})^3$ be the three-dimensional torus with sides identified. That is, I am considering the unit box $[0,1]^3$ with periodic boundary conditions.
In this case, I am (hopefully) trying to find an explicit formula for the Green function for the Laplacian $-\Delta$.
That is, what would a function $G$ on $\mathbb{T}^3$ satisfying $-\Delta G(x)=\delta^3(x)$ look like explicitly?
I am aware that on whole $\mathbb{R}^3$, $G(x)= \frac{1}{4\pi \lvert x \rvert}$.
According to standard PDE references, I think I need to find the corrector function $\phi^y(x)$ defined by \begin{equation} -\Delta_x \phi^y(x)=0 \text{ for } x \in (0,1)^3 \text{ and } \phi^y(x)=\frac{1}{4\pi \lvert x-y \rvert} \text{ for } x \in \partial \mathbb{T}^3 \end{equation} together with $y \in \mathbb{T}^3$ and $y \neq x$.
However, I have great difficulty solving the above Poisson equation, and moreover, I am not sure if the resulting $\phi^y(x)$ will even be a periodic function.
Could anyone please help me?
Edit: I forgot the fact that the periodic boundary conditions allow zero modes and the Laplacian does not have an inverse under this condition. So, I am restricting the domain of the Laplacian to $L^2$ space over $\mathbb{T}^3$ with no zero modes. Then will it make a difference?