In this case, since masses of both charges are not the same, we need to find center of mass (COM), about which dipole will oscillate and then we will find moment of inertia about this axis, to find torque and hence angular frequency \( \omega \).
Given, the mass of positive charge is \(m\), so the center of mass will be at a distance \(L\) from the negative charge:
\[
\frac{L}{3} = \frac{2m}{3m} = \frac{2L}{3}
\]
The moment of inertia about the axis is \(I = \frac{2mL^2}{3}\). Hence, angular frequency:
\[
\omega = \sqrt{\frac{qE}{I}} = \frac{4qE}{3ml}
\]