Step 1: Using Energy Conservation
The total mechanical energy of the particle is:
\[
E = \frac{1}{2} m v^2 - \frac{GMm}{R}
\]
For escape velocity:
\[
v_e = \sqrt{\frac{2GM}{R}}
\]
Step 2: Applying Given Condition
The initial velocity given is \( v = 2v_e \):
\[
E = \frac{1}{2} m (4 v_e^2) - \frac{GMm}{R}
\]
Substituting \( v_e^2 = \frac{2GM}{R} \):
\[
E = 2GMm/R - GMm/R = GMm/R
\]
At infinity, kinetic energy remains:
\[
\frac{1}{2} m v_{\infty}^2 = GMm/R
\]
Solving for \( v_{\infty} \):
\[
v_{\infty} = \sqrt{3} v_e
\]
Thus, the correct answer is option (3).