In optics, Fraunhofer diffraction or far-field diffraction is diffraction of light through an aperture, or slit, for small values of the Fresnel number, . It is also known as parallel beam diffraction. This corresponds to the observation of diffraction on a system (aperture, grating, slit, etc.) which is at large distance both from the source and the screen (where the interference pattern is observed). Essentially the same situation takes place when the optical system is sandwiched by a pair of positive lenses with the source and the screen at their foci.
The far-field diffraction pattern of a source may also be observed (except for scale) in the focal plane of a well-corrected lens. The far-field pattern of a diffracting screen illuminated by a point source may be observed in the image plane of the source.
If a light source and an observation screen are effectively far enough from a diffraction aperture (for example a slit), then the wavefronts arriving at the aperture and the screen can be considered to be collimated, or plane. Fresnel diffraction, or near-field diffraction occurs when this is not the case and the curvature of the incident wavefronts is taken into account.
In far-field diffraction, if the observation screen is moved relative to the aperture, the diffraction pattern produced changes uniformly in size. This is not the case in near-field diffraction, where the diffraction pattern changes both in size and shape.
Since this type of diffraction is mathematically simple, this experimental setup can be used to find the wavelength of the incident monochromatic light with high accuracy.
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"Fraunhofer diffraction".
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