I am confused by conjugation, and the action of group elements on themselves. If I have a rotation acting on the generators of $su(2)$, i.e.
\begin{align} R_\theta (L_1, L_2, L_3) \end{align}
where $R_\theta$ is some rotation matrix. The elements of the vector $(L_1, L_2, L_3)$ are themselves the $su(2)$ generators, in an $N$-dimensional representation. Is it true that this action can be equivalently stated as a conjugation of the elements themselves? i.e.
\begin{align} R_\theta (L_1, L_2, L_3) \leftrightarrow (\Omega L_1 \Omega^\dagger, \Omega L_2 \Omega^\dagger, \Omega L_3 \Omega^\dagger) \end{align}
where $\Omega$ is defined by, for the example of a rotation around the $z$-axis,
$$\Omega = e^{i\theta L_3}$$