Concept:
The stiffness of a beam is defined as the moment required to produce unit rotation while keeping all other joints fixed.
For a beam member of length \(l\) fixed at both ends, the rotational stiffness at one end is
\[
k=\frac{4EI}{l}.
\]
When a moment is applied at the centre of a beam fixed at both ends, the beam is divided into two equal spans.
Step 1: Determine the length of each half.
The total beam length is
\[
2L.
\]
Hence, each half has length
\[
L.
\]
Step 2: Find the stiffness of each half.
Each half behaves as a beam fixed at one end and connected to the centre.
Therefore,
\[
k=\frac{4EI}{L}.
\]
Step 3: Compute the total stiffness at the centre.
Since two identical beam segments meet at the centre, their stiffnesses act in parallel.
Hence,
\[
k_{\text{total}}
=
\frac{4EI}{L}
+
\frac{4EI}{L}
=
\frac{8EI}{L}.
\]
Thus, the moment required for unit rotation at the centre is
\[
\boxed{\frac{8EI}{L}.}
\]
Therefore, the correct option is
\[
\boxed{(D)\;\dfrac{8EI}{L}.}
\]