Step 1: Understanding the Concept:
Rotational KE is \(\frac12I\omega^2\). With equal KE, \(I_A\omega_A^2 = I_B\omega_B^2\), so \(\frac{\omega_B}{\omega_A} = \sqrt{\frac{I_A}{I_B}}\).
Step 2: Moments of inertia:
Ring A about its diameter: \(I_A = \frac12MR^2\).
Ring B about a tangent in its plane: use the parallel axis theorem, \(I_B = \frac12MR^2 + MR^2 = \frac32MR^2\).
Step 3: Ratio:
\[ \frac{\omega_B}{\omega_A} = \sqrt{\frac{\frac12MR^2}{\frac32MR^2}} = \sqrt{\frac13} = \frac{1}{\sqrt3} \]
So \(\omega_B : \omega_A = 1 : \sqrt3\).
Step 4: Why the other options are wrong.
The ratio 1:3 comes from forgetting the square root. Options (C) and (D) involve 2, as if a different moment of inertia such as \(MR^2\) was used for one of the rings.
Final Answer:
The ratio is \(1 : \sqrt3\), option (B).
\[ \boxed{1:\sqrt{3}} \]