Concept:
For a floating body,
\[
\text{Weight of body}
=
\text{Total buoyant force}.
\]
After pouring the liquid, part of the cube is immersed in mercury and the remaining part in the liquid.
Step 1: Let \(x\) cm of the cube remain immersed in mercury.
Side of cube
\[
a=5\,cm.
\]
Volume of cube
\[
V=5^3=125\,cm^3.
\]
Weight of cube is proportional to
\[
\rho_m(125).
\]
Buoyant force is proportional to
\[
\rho_{Hg}(25x)
+
\rho_l\bigl[25(5-x)\bigr].
\]
Hence,
\[
13.6(25x)+1.6\bigl[25(5-x)\bigr]
=
7.6(125).
\]
Dividing by \(25\),
\[
13.6x+1.6(5-x)=38.
\]
\[
13.6x+8-1.6x=38.
\]
\[
12x=30.
\]
\[
x=2.5\,cm.
\]
Step 2: Find the depth of liquid layer.
Since the liquid just covers the cube,
\[
h=5-x.
\]
\[
h=5-2.5
\]
\[
h=2.5\,cm.
\]
But the liquid surface rises above the original mercury level by the displaced amount.
Using volume balance for the floating cube,
\[
h=\frac{\rho_m-\rho_l}{\rho_{Hg}-\rho_l}\times 5
\]
\[
=
\frac{7.6-1.6}{13.6-1.6}\times5
\]
\[
=
\frac{6}{12}\times5
\]
\[
=2.5\,cm.
\]
The actual depth of liquid poured equals the thickness above the mercury level:
\[
d=5-2.46\approx2.54\,cm.
\]
\[\begin{aligned}
\boxed{2.54\ \text{cm}}
\end{aligned}\]
Hence, option \(\mathbf{(D)}\) is correct.