For a parallel plate capacitor partially filled with a dielectric, the equivalent capacitance is given by:
\[
C = \frac{\varepsilon_0 A}{d} \frac{1}{\frac{x}{\kappa} + (1-x)}
\]
where:
- \( x \) is the fraction of the dielectric-filled space,
- \( \kappa \) is the dielectric constant.
1. Case 1: Half-filled (\( x = \frac{1}{2} \), \( \kappa = 4 \))
\[
\frac{1}{C_1} = \frac{1}{C_0} \left(\frac{1}{\frac{1}{2 \times 4} + \frac{1}{2}} \right)
\]
\[
\frac{1}{C_1} = \frac{1}{C_0} \left(\frac{1}{\frac{1}{8} + \frac{1}{2}} \right)
\]
\[
C_1 = \frac{8}{5} C_0
\]
2. Case 2: One-third filled (\( x = \frac{1}{3} \), \( \kappa = 4 \))
\[
\frac{1}{C_2} = \frac{1}{C_0} \left(\frac{1}{\frac{1}{3 \times 4} + \frac{2}{3}} \right)
\]
\[
\frac{1}{C_2} = \frac{1}{C_0} \left(\frac{1}{\frac{1}{12} + \frac{2}{3}} \right)
\]
\[
C_2 = \frac{6}{5} C_0
\]
3. Ratio of \( C_1 : C_2 \):
\[
\frac{C_1}{C_2} = \frac{8}{5} C_0 : \frac{6}{5} C_0 = 6:5
\]
Thus, the correct answer is \(\boxed{6:5}\).