Doing the cov $z = z_0 + \rho e^{i\theta}$,
$$
\iint_{|z-z_0|\le\rho}|f(z)|^2\,dxdy = \int_0^\rho\!\int_0^{2\pi}|f(z)|^2r\,d\theta dr = \int_0^\rho\!\int_0^{2\pi}\left(\sum_{n=0}^{\infty}a_{n}r^n e^{in\theta}\right)
\overline{\left(\sum_{n=0}^{\infty}a_{n}r^n e^{in\theta}\right)}r\,d\theta dr
$$
$$
= \int_0^\rho\!\int_0^{2\pi}\left(\sum_{j=0}^{\infty}a_{j}r^j e^{ij\theta}\right)
\left(\sum_{k=0}^{\infty}\overline{a_{k}}r^k e^{-ik\theta}\right)r\,d\theta dr =
$$
$$
= \int_0^\rho\!\int_0^{2\pi}\left(\sum_{n=0}^{\infty}
\left(\sum_{j+k=n}a_{j}\overline{a_{k}}e^{i(j-k)\theta}\right)r^{n+1}\right)d\theta dr.
$$
Because of the periodicity of imaginary exponential, the terms with $j\ne k$ give $0$. On the other hand, $j = k$ implies $e^{i(j-k)\theta} = 1$ and $j + k$ even, so:
$$
\iint_{|z-z_0|\le\rho}|f(z)|^2\,dxdy = 2\pi\int_0^{\rho}\sum_{n=0}^{\infty}
|a_n|^2 r^{2n+1}dr = 2\pi\sum_{n=0}^{\infty}
|a_n|^2\frac{\rho^{2n+2}}{2n+2}.
$$