The expression is a scalar diffraction theory integral for a monochromatic wave. The complex quantity represents a field complex amplitude, with physical field obtained by taking the real part after multiplication by . The light intensity is proportional to . The coordinates label transverse positions in the aperture plane, is its transmitting region, and is the incident field multiplied by the aperture's complex transmission. The wavenumber is in the propagation medium, and is the axial propagation distance if already includes the incident field.
To derive the Fresnel diffraction, start from Huygens-Fresnel principle contributions with propagation factor . With the coordinate origin at the projection of into the aperture plane,
The paraxial approximation requires , where . Replace the slowly varying and the obliquity factor by their axial values, but retain the quadratic variation of wave phase. Neglect of the next wave phase term requires over the relevant aperture. Thus, apart from a common constant,
The quadratic wave phase may be of order one or much larger; setting it to zero would require the stronger conditions for Fraunhofer diffraction. The scalar treatment also neglects the detailed vector field at aperture edges and assumes dimensions large enough compared with wavelength for this approximation to be useful.
For a finite-distance axial point source at distance and an observer at distance , the incident field contributes its own quadratic wave phase. If instead denotes only the aperture transmission, the combined curvature is described by an effective distance
These are two equivalent conventions for distributing the incident wave phase between and the exponential. Both distances must be included in the later calculation.

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