Concept:
For a one-dimensional collision,
\[
e=
\frac{\text{Relative velocity of separation}}
{\text{Relative velocity of approach}}.
\]
Also, linear momentum is conserved.
Step 1: Apply conservation of momentum.
Let the initial velocity of ball \(A\) be
\[
u.
\]
Since ball \(B\) is at rest,
\[
u_B=0.
\]
Let final velocities be
\[
v_A=v,
\qquad
v_B=2v.
\]
Since the masses are identical,
\[
mu=m v_A+m v_B.
\]
\[
u=v+2v.
\]
\[
u=3v.
\]
\[
v=\frac{u}{3}.
\]
Therefore,
\[
v_A=\frac{u}{3},
\qquad
v_B=\frac{2u}{3}.
\]
Step 2: Use the definition of coefficient of restitution.
\[
e
=
\frac{v_B-v_A}{u_A-u_B}.
\]
Substituting,
\[
e
=
\frac{\frac{2u}{3}-\frac{u}{3}}
{u-0}.
\]
\[
=
\frac{\frac{u}{3}}{u}.
\]
\[
=
\frac13.
\]
Therefore,
\[
\boxed{e=\frac13}
\]
\[
\boxed{\text{Answer = (A)}}
\]