While reviewing some lecture notes, I stumbled upon the following proposition. $\newcommand{\vertiii}[1]{{\left\vert\kern-0.25ex\left\vert\kern-0.25ex\left\vert #1 \right\vert\kern-0.25ex\right\vert\kern-0.25ex\right\vert}}$
Let $\Omega \subset \mathbb{R}^d$ be a bounded Lipschitz domain and consider the Sobolev space $H^1 (\Omega) := W^{1,2}(\Omega)$. Then the following norms are equivalent on $H^1 (\Omega) $: \begin{align} \Vert v \Vert_1^2 &:= \int_\Omega v^2 dx + \int_{\Omega} \vert \nabla v \vert^2 dx =: \Vert v \Vert_0^2 + \vert v\vert_1^2 \\ \vertiii{v}_1^2 &:= \int_{\partial \Omega} v^2 d\sigma + \vert v \vert_1^2 \end{align}
Showing this proposition consists of applying a theorem, that was stated without proof:
Let $\lbrace f_i \rbrace_{i=1}^l$ be a system with the properties
- $f_i : H^1(\Omega) \rightarrow \mathbb{R}_0^+$ is a semi norm
- $\exists C_i >0$ s.t. $0 \leq f_i(v) \leq C_i \Vert v \Vert_1 \quad \forall v \in H^1 (\Omega)$
- $f_i$ is a norm on the polynomials of degree $0$
then the $\Vert \cdot \Vert_1$-norm and \begin{equation} \vertiii{v}^2 := \sum\limits_{i=1}^l f_i^2(v) + \vert v \vert_1^2 \end{equation} are equivalent.
Proving that $f_1(v) := \int_{\partial \Omega} v^2 d\sigma$ indeed possesses the properties of the theorem is straight forward (continuity of the trace operator for boundedness, ...). However, I am interested in the proof of the theorem itself.
I would be grateful for references in the literature, hints for doing the proof myself or comments.