The N-slit interferometer is an extension of the double-slit interferometer also known as Young's double-slit interferometer. One of the first known uses of N-slit arrays in optics was illustrated by Newton.[1] In the first part of last century, Michelson[2] described various cases of N-slit diffraction.
Feynman[3] described thought experiments, of two-slit quantum interference, of electrons using Dirac's notation.[4] This approach was extended to N-slit interferometers, by Duarte and colleagues in 1989,[5] using narrow-linewidth laser illumination, that is, illumination by indistinguishable photons. The first application of the N-slit interferometer was the generation and measurement of complex interference patterns.[5][6] These interferograms are accurately reproduced, or predicted, by the N-slit interferometric equation for either even (N = 2, 4, 6,…), or odd (N = 3, 5, 7,…), numbers of slits.[6]
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The N-slit laser interferometer, introduced by Duarte[5][6][7], uses prismatic beam expansion to illuminate a transmission grating, or N-slit array, and a photoelectric detector array (such as a CCD or CMOS) at the interference plane to register the interferometric signal.[6][7][8] The expanded laser beam illumination in the N-slit interferometer can also take the shape, via the introduction of a convex lens prior to the prismatic expander, of a beam extremely elongated in the propagation plane and extremely thin in the orthogonal plane.[6][7] This use of one-dimensional (or line) illumination eliminates the need of point-by-point scanning in microscopy and microdensitometry.[6][7] Thus, these instruments can be used as straight forward N-slit interferometers or as interferometric microscopes (see section on microscopy).
These interferometers, originally introduced for applications in imaging,[6] are also useful in optical metrology and have been proposed for secure optical communications in free space.[9] Recent experimental developments include intra-interferometric path lengths of 35 meters[10] and 527 meters.[11]
These large, and very large, N-slit interferometers[10][11] are also being used to study the effect of intra interferometric clear air turbulence[10] and the effect of microscopic disturbances[11] on propagating interferometric signals. This work has yielded the first observation of diffraction patterns superimposed over propagating interferograms.[11]
These diffraction patterns (as shown in the first photograph) are generated by inserting a spider web fiber (or spider silk thread) into the propagation path of the N-slit interferogram. The position of the spider web fiber is perpendicular to the plane of propagation.[11]
Note: N-slit interferometers include three-slit interferometers (or triple-slit interferometers), four-slit interferometers, etc.[9][10][11]
As previously mentioned the original application of the N-slit laser interferometer was interferometric imaging.[6][7][12] In particular, the one dimensionally expanded laser beam (with a cross section 25-50 mm wide by ~25 μm high) was used to illuminate imaging surfaces (such as silver-halide films) to measure the microscopic density of the illuminated surface. Hence the use of the description interferometric microdensitometer.[7] Resolution down to the nano regime can be provided via the use of interinterferometric calculations.[6]
The multiple-prism expanded laser beam is also described as an extremely elongated laser beam. The elongated dimension of the beam (25-50 mm) is in the plane of propagation while the very thin dimension (~25 μm) of the beam is in the orthogonal plane. This was demonstrated, for imaging and microscopy applications, in 1993.[6][7] Alternative descriptions of this type of extremely elongated illumination might include the terms line illumination, linear illumination, thin light sheet illumination, and plane illumination.
N-slit interferometers are also of interest to researchers working in atom optics,[13] Fourier imaging,[14] and quantum computing.[15]
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