Let $\mathbb{T}^3:=(\mathbb{R}/\mathbb{Z})^3$ be the $3$-torus and $C^\infty(\mathbb{T}^3,\mathbb{R}^3)$ be the Frechet space of smooth periodic vector fields on $\mathbb{T}^3$.
By Helmholtz decomposition (or Hodge's Theorem), each $f \in C^\infty(\mathbb{T}^3,\mathbb{R}^3)$ is uniquely written as \begin{equation} f(x)=a+g(x)+h(x) \end{equation} where $a \in \mathbb{R}^3$ is a constant vector while $g, h \in C^\infty(\mathbb{T}^3,\mathbb{R}^3)$ satisfy
- $\int_{\mathbb{T}^3}g=\int_{\mathbb{T}^3}h=0$
- $\nabla \times g = 0$, that is $g$ is curl-free
- $\nabla \cdot h=0$, that is $h$ is divergence-free
Now, the Leray projection $\mathbb{P}$ is a linear map on $C^\infty(\mathbb{T}^3,\mathbb{R}^3)$ defined by \begin{equation} \mathbb{P}f= h \end{equation}
Now, I wonder if this $\mathbb{P}$ is continuous with respect to the Frechet topology of $C^\infty(\mathbb{T}^3,\mathbb{R}^3)$. I am concerned with this issue because the seminorms on $C^\infty(\mathbb{T}^3,\mathbb{R}^3)$ contain supremums, and usual Fourier expansion is not (equi-)continuous with respect to $L^\infty$-norm..
Could anyone pleaes clarify for me?