Step 1: Find the intensity after the first polaroid.
Let the intensity of the unpolarized light incident on \(Q\) be
\[
I_0.
\]
After passing through \(Q\),
\[
I_1=\frac{I_0}{2}.
\]
This is the intensity incident on the middle polaroid \(P\).
Step 2: Apply Malus' law.
For maximum transmitted intensity through two crossed polaroids, the axis of \(P\) should make an angle
\[
45^\circ
\]
with each polaroid.
After passing through \(P\),
\[
I_2
=
I_1\cos^245^\circ
=
\frac{I_1}{2}.
\]
After passing through \(R\),
\[
I_3
=
I_2\cos^245^\circ
=
\frac{I_1}{4}.
\]
Since
\[
I_1=\frac{I_0}{2},
\]
we get
\[
I_3=\frac{I_0}{8}.
\]
Step 3: Find the required ratio.
The intensity incident on \(P\) is
\[
I_1=\frac{I_0}{2}.
\]
The intensity emerging from \(R\) is
\[
I_3=\frac{I_0}{8}.
\]
Therefore,
\[
I_1:I_3
=
\frac{I_0}{2}:\frac{I_0}{8}
=
4:1.
\]
Hence,
\[
\boxed{4:1}.
\]
Thus,
\[
\boxed{(A)}
\]
is the correct answer.