The following is from Linear Integral Equations by Kress.
- Should definition $1.4$ read that "...if each sequence converging ${\color{red}{\text{to } x \in X}}$ with respect to the first norm also converges ${\color{red}{\text{to the same }x}}$ with respect to the second norm and vice versa."
- In the Proof of Theorem $1.5$ for the second part, how to prove that if there is no $C \in \mathbb{R}$, then there exists a sequence $(\phi_n)$ with $\Vert \phi_n\Vert_a = 1$ and $\Vert \phi_n \Vert_b \geq n^2$? Is the following the right way to think about?
We will prove that if there doesn't exist $c, C\in \mathbb{R}$ such that $$c\Vert{\phi}\Vert_a \leq \Vert{\phi}\Vert_b \leq C\Vert{\phi}\Vert_a$$ for all $\phi \in X$, then the two norms $\Vert{\cdot}\Vert_a$ and $\Vert{\cdot}\Vert_b$ are not equivalent. Since there doesn't exist constants $c$ and $C$, this means there exists a sequence of $\phi_n \in X$, such that $\dfrac{\Vert{\phi_n}\Vert_b}{\Vert{\phi_n}\Vert_a} \geq n^2$. Consider the sequence $\psi_n = \dfrac1n \cdot \dfrac{\phi_n}{\Vert{\phi_n}\Vert_a}$. We then have $\Vert{\psi_n}\Vert_a = \dfrac1n$ and $\Vert{\psi_n}\Vert_b \geq n$. This means $\lim_{n \to \infty} \Vert{\psi_n}\Vert_a = 0$, whereas $\lim_{n \to \infty} \Vert{\psi_n}\Vert_b \geq n$. Hence, $\psi_n \to 0$ in $\Vert{\cdot}\Vert_a$, whereas $\psi_n$ doesn't converge to $0$ in $\Vert{\cdot}\Vert_b$.