The phenomenon observed is the phenomenon of diffraction
(i) At the central maxima. The contribution due to the secondary wavelets, from all parts of the wavefront (at the slit), arrive in phase at the central maxima θ = o
At the secondary maxima
It is only the contribution from (nearly) 1/3 (or 1/5, or 1/7,...) of the secondary maxima. These occur at points for which
At the minima
The contribution, from 'corresponding pairs', of the sub-parts of the incident wavefront, cancel each other and the net contribution, at the location of the minima, is zero. The minima occur at points for which
(ii) There is a significant fall in intensity at the secondary maxima because the intensity there, is only due to the contribution.n o{ (nearly) (1/3 or 1/5 or 1/7,....) of the incident wavefronts.
(iii) The size of the central maxima would get halved when width of the slit is doubled.