We begin with an integral from zero to pi of a function of the angle [itex]\theta[/itex].
Using x = cos ([itex]\theta[/itex].) visibility of the fringes becomes
[itex]A\int_{-1}^1 (1+x^2) e^{i u x} dx[/itex].
Integrating it twice by parts we get
[itex]4A [\frac{sin u}{u}+\frac{cos u}{u^2}-\frac{sin u}{u^3}][/itex].
"u" being the distance of slits divided by the wavelength of the photon when it decreases to zero the limit of visibility must be 1. We need so a normalization factor and the good formula is
[itex]3/2 [\frac{sin u}{u}+\frac{cos u}{u^2}-\frac{sin u}{u^3}][/itex].
We can compute the visibility when u = 1. It is when we watch the electrons with light having for wavelength the distance
between the slits. We have V(1) = 3/2 cos(1) = 0.8
So the visibility is still very good!