Step 1: Understanding the relation.
The angular frequency \( \omega \) for a rotating molecule is related to the rotational kinetic energy by the formula:
\[
E = \frac{1}{2} I \omega^2
\]
where \( I \) is the moment of inertia. For a diatomic molecule, \( I = \mu r^2 \), where \( \mu \) is the reduced mass and \( r \) is the distance between the atoms.
Step 2: Using the given values.
Substitute \( I = \mu r^2 \) and \( \mu = \frac{m}{2} \), and solve for the angular frequency \( \omega \). After simplification, we obtain:
\[
\omega = \frac{2}{d} \sqrt{\frac{E}{m}}
\]
Step 3: Conclusion.
Thus, the angular frequency is \( \frac{2}{d} \sqrt{\frac{E}{m}} \), which corresponds to option (A).