Huygens principle says that you can represent any wave front by an infinite number of secondary wavelets, placed along the front. That's the fundamental principle behind Diffraction theory; the wavelets are not 'real', they're just an aid to calculation - just like all calculations which involve integration. The basic Young's Interference from two slits treats each slit as just one wavelet. This is ok for predicting the positions of the peaks and troughs of the interference pattern near the boresight. But a slit of finite width will not have the isotropic pattern of a single wavelet so, if you want to predict the actual pattern, you need to take the pattern of a finite width slit. When the slits (or a number off slits) are identical, the overall pattern is the pattern of one slit multiplied by the interference pattern of the idealised point sources. See those images further up. Very wide slits send most of the light in the forward direction which swamps the visibility of the side peaks.
In practice, there's a compromise between having slits that are wide enough to get a bright pattern but not so wide that the brightness of the side fringes drops off so that you lose the pattern.