Step 1: Understanding potential energy in S.H.M.
In Simple Harmonic Motion (S.H.M.), the potential energy at a displacement \( x \) is given by:
\[
U = \frac{1}{2} k x^2
\]
Where \( k \) is the spring constant and \( x \) is the displacement from the equilibrium position.
Step 2: Using the given displacements.
At displacement \( x_1 \), the potential energy is \( U_1 = \frac{1}{2} k x_1^2 \), and at displacement \( x_2 \), the potential energy is \( U_2 = \frac{1}{2} k x_2^2 \).
For the displacement \( x_1 + x_2 \), the potential energy will be:
\[
U = \frac{1}{2} k (x_1 + x_2)^2
\]
Thus, the potential energy at the combined displacement is represented by the sum of the individual potential energies, hence the correct answer is (A) \( \sqrt{U_1} + \sqrt{U_2} \).