Equation 180 of Aravos' notes gives: $$t(\mathbf{d})\psi(\mathbf{r})t^\dagger(\mathbf{d})=\psi(\mathbf{r}+\mathbf{d})$$
Where $t(\mathbf{d})$ is the magnetic translation operator. Why does this operator act on both sides of the state? It makes sense if it was an operator instead of a state because then if it acted on a translated state, it would be untranslated, acted on by the operator in the untranslated basis, then translated back.
Or is this just an overuse of notation where $\psi$ doesn't represent a state $\left|\psi\right>$ with the $\mathbf{r}$ showing that it is untranslated and not in a basis?