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Diffraction by N-slits
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Optical disturbance due to N slits
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Irradiance due to N-slits I 0 = I rradiance by single slit at =0
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For principal maxima or
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For minima Between consecutive principal maxima, there will be N-1 minima
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Subsidiary maxima (N-2) subsidiary maxima between consecutive principle maxima
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For large N, irradiance of first subsidiary maxima
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Diffraction from multiple slits Slit Diffraction Pattern
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Normal incidence Transmission grating
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Oblique incidence a
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For two wavelengths
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Grating in spectroscopy Identification of element
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Dispersive power of grating Width of principal maxima
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Barely resolved ItIt s w
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Chromatic resolving power of a grating
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Chromatic resolving power of a prism
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Reflection grating
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Diffraction grating
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The nominal track separation on a CD is 1.6 micrometers, corresponding to about 625 tracks per millimeter. This is in the range of ordinary laboratory diffraction gratings. For red light of wavelength 600 nm, this would give a first order diffraction maximum at about 22°.
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15 15 0 nm 450 nm Atomic Force Microscope Image of CD
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Phase grating Delta function Bessel function
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Bragg’s law X-ray diffraction from crystals: 2d Sin θ = n λ
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Electron diffraction patterns of a real 3D quasicrystal. The periodic structure of a crystalline solid acts as a diffraction grating, scattering the electrons in a predictable manner. Working back from the observed diffraction pattern, it may be possible to deduce the structure of the crystal producing the diffraction pattern.
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1. Optics Author: Eugene Hecht Class no. 535 HEC/O Central library IIT KGP
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