The moment of inertia of a square plate of length $2l$ and mass $m$ about an axis at its centre and perpendicular to its plane is $\frac{1}{12}m((2a)^2+(2a)^2)$. The particle has moment of inertia $3m(\sqrt2a)^2$.
Thus $$\frac23ma^2\omega = \left(\frac23ma^2 +6ma^2\right)\omega' =\frac{20}{3}ma^2\omega'$$ where $\omega'$ is the final angular velocity. Dividing both sides by $\frac{20}{3}ma^2$ gives the desired answer.