[size=85] In the half-wave slit model, the near-field (Fresnel) diffraction field behind a slit ([b]b = 6[/b], [b]λ = 1[/b]) is structured by a family of continuous [i]extremal[/i] (or [i]stationary[/i]) lines. The intersections of these lines correspond to critical points ([b]local maxima[/b], [b]minima[/b], or [b]saddle[/b] points) in the intensity distribution[b] J(x, y)[/b], which define the [b][i]exact conditions[/i][/b] for [b][i]destructive[/i][/b] and [b][i]constructive[/i][/b] [b]interference[/b] of waves from half-wave zones.[/size]