The Hamiltonian is given as
$H=-\frac{\hbar^2}{2 m_e r^2}\displaystyle\sum_{n=1}^N \dfrac{\partial^2}{\partial \theta_n^2}$
In the first part we show that the $\psi_k=\frac{1}{\sqrt{2\pi}}\exp(i k \theta)$ is a solution to $H\psi_k = E_k \psi_k$.
$E_k=\frac{k^2 \hbar^2}{2 m_e r^2}$
All fine so far.
$r$ is given to be $4 \times 10^{-10}\text{m}$ and $N=18$ and it asks for the ground state energy.
I am unsure how the $k=0$ state can be occupied since zero energy is forbidden?
But for each quantum number $k=0,\pm 1,\pm 2\cdots$ we have an increasing energy so the ground state will consist of
$(k=0)^2(k=1)^2(k=-1)^2(k=2)^2(k=-2)^2(k=3)^2(k=-3)^2(k=4)^2(k=-4)^2$
Where $(k=0)^2$ denotes 2 electrons being in the state with $k=0$, one with spin up and one with spin down.
The corresponding energy: $\displaystyle\sum_{k=-4}^4 2E_k = \frac{60 \hbar^2}{m_e r^2} = 4.57 \times 10^{-18} \text{J}$
But in the solution the energy is given as $\frac{30 \hbar^2}{m_e r^2} = 2.29 \times 10^{-18} \text{J}$, half of my value. Is this an error or have I missed something?