Energy stored in the electric field or self energy of a solid sphere of radius $r$ and uniform charge distribution $q$ would be $$\frac{3}{5}\frac{1}{4\pi\epsilon_0}\frac{q^2}{r}$$
This result could be derived if we take electrostatic energy density $u = \frac{1}{2}\epsilon_0{E^2}$ where $E$ is the electric field intensity. From work-energy theorem, this energy would be the total work done to configure this uniformly charged solid sphere from infinity. Since the charge is quantised, $q=ne$ where $e$ is charge of an electron. If $dq=e$ quantised charged units are assembled from infinity, work done on the system gets stored in the electric field.
But when $n=1$ and if we consider it to be an electron with its classical radius, we get the value of self energy as $$\frac{3}{5}\frac{1}{4\pi\epsilon_0}\frac{e^2}{r}$$ Or at least we get something very finite.
I don't understand if this is the energy stored in the electric field and if so, is it intrinsic because with one $e$ charge, work-energy theorem doesn't make sense here. Or what about the error(s) in the assumptions leading to it?
Edit: I have come across this Wikipedia article (that I should have stumbled upon before asking here) and it happens to address most of my doubts (and inconsistencies).