In Folland's real analysis, it writes
Nonexample: Let $\mu$ be Lebesgue measure and $\upsilon$ the point mass at 0 on $(\mathbb{R}, \mathcal{B}_{\mathbb{R}})$. Clearly $\upsilon \perp \mu$. The nonexistent Radon-Nikodym derivative $dv/d\mu$ is popularly known as the Dirac $\delta$-function.
I'm confused why is the Radon-Nikodym derivative $dv/d\mu$ said to be nonexistent? Isn't it just the Dirac $\delta$-function as the author later said?
Any help would be appreciated!