It's not called the uncertainty relation for nothing, then

.
The outcomes aren't all that irreconcilable: if the exercise asks what's true for the majority of the electrons, then this carefully selected collection of electrons will indeed satisfy what you call 2 (<, formerly option C -- as you see, you yourself also contribute a little bit to the confusion

).
And we are into interpretation issues if we defend option 3 (##\approx##, formerly A:) which as Fowler works out, is true for the whole lot -- which is an even greater majority. The other two options (> and >>) can be ruled out.
If I were you, I wouldn't spend too much energy on this: it's simply not a very good question. Fowler (and you, and me too, and many others with us) would pick ##\approx## without hesitation. (Unless your challenging means the difference between pass or fail, in which case showing a genuine interest and a sensible defence of your choice may make a good impression and change the balance in you favour)
I would also like to point out that I strongly oppose the notion suggested in post #22:
The problem suggests that the electron in passing through the slit receive an impulse of Δp but I believe that interpretation is not warranted.
The question statement does not -- and does not have to -- suggest that at all. This whole slit business is about the wave character of the electrons: they really, intrinsically and fundamentally exhibit wave behaviour, which means that after a slit there is a diffraction pattern, even if before the slit the beam is exactly parallel (meaning infinitely wide by the same Heisenberg relation!). And the majority does end up in the central maximum.