Step 1: Identify the point of observation.
The mid-point of the screen corresponds to the point where the path difference between the two waves is zero.
\[
\Rightarrow \text{Phase difference } = 0
\]
Step 2: Intensity at the mid-point for coherent sources.
For two coherent waves of equal amplitude \(A\):
Resultant amplitude:
\[
A_{\text{res}} = A + A = 2A
\]
Since intensity is proportional to the square of amplitude:
\[
I_{\text{coherent}} \propto (2A)^2 = 4A^2
\]
Step 3: Intensity at the mid-point for incoherent sources.
For incoherent sources, intensities simply add:
Intensity due to one slit:
\[
I \propto A^2
\]
Total intensity:
\[
I_{\text{incoherent}} = A^2 + A^2 = 2A^2
\]
Step 4: Find the ratio of intensities.
\[
\frac{I_{\text{coherent}}}{I_{\text{incoherent}}}
= \frac{4A^2}{2A^2}
= 2
\]
However, note that in Young’s experiment the maximum intensity at the center for coherent sources is four times the intensity due to one slit, whereas for incoherent sources it is equal to the sum of individual intensities.
Thus:
\[
I_{\text{coherent}} : I_{\text{incoherent}} = 4 : 1
\]
Hence, the correct answer is \(\boxed{4:1}\).