Let $M$ be an oriented, compact, finite-dimensional Riemannian manifold and let $\Omega^k$ denote the space of differential $k$-forms on $M$. Endow $\Omega^k$ with its usual Fréchet topology (where differential forms are seen as sections of a exterior product bundle). Denote the Fréchet space of vector fields on $M$ by $\mathcal{X}$.
Are the following operations on differential forms continuous?
- Wedge product: $\wedge: \Omega^k \times \Omega^l \to \Omega^{k+l}$
- Contraction: $\iota: \mathcal{X} \times \Omega^k \to \Omega^{k-1}$
- Exterior derivative: $d: \Omega^k \to \Omega^{k+1}$
- Hodge star: $\star: \Omega^k \to \Omega^{n-k}$
- Integration: $\int_M: \Omega^n \to \mathbb{R}$
The wedge product, contraction and the Hodge star should be continuous because they arise from fibre-preserving operations on the underlying bundles (correct?). What about the derivative and integration?
Side-question/remark: If all these operations are continuous, then the map $\Omega^k \to \mathbb{R}$ defined by $\alpha \mapsto \int_M \alpha \wedge \star \alpha$ would be a continuous norm on $\Omega^k$, which I suspect is in contradiction to the fact that the topology on $\Omega^k$ is defined by a family of seminorms.