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En [[óptica]], una '''rede de difracción''' ye un [[preséu ópticu|componente ópticu]] con un patrón regular, qu'estrema ([[difracción|difracta]]) la lluz en dellos fexes de lluz que viaxen en distintes direccionesdireiciones. Les direccionesdireiciones d'esos fexes de lluz dependen del espaciado de la rede y de la [[llargor d'onda]] de la lluz incidente, de cuenta que la rede actúa como un elementu dispersivo. Gracies a esto, les redes utilícense davezu en [[monocromador]]es y [[espectrómetru|espectrómetros]].
 
== Tipu Echelle ==
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== Principle ==
The intensity of the diffraction pattern can be altered by tilting the grating. Especially with reflective gratings (where the holes are replaced by a highly reflective surface), the reflective portion can be [[Blazed grating|tilted (blazed)]] to scatter a majority of the light into the preferred direction of interest (specific diffraction order).
For multiple wavelengths the same is true; however, there it is possible that longer wavelengths of a higher order might overlap with the next order(s) of a shorter wavelength, which usually is an unwanted side effect.
 
In echelle gratings, however, this behaviour is deliberately used and the [[blaze]] is optimized for multiple overlapping higher orders. Since this overlap is not directly useful, a second, perpendicularly mounted dispersive element ([[grating]] or [[prism (optics)|prism]]) is inserted as an "order separator" or "cross disperser" into the beam path. Hence the spectrum consists of stripes with different, but slightly overlapping, wavelength ranges that run across the imaging plane in an oblique pattern.
Exactly this behaviour helps to overcome imaging problems with broadband, high-resolution spectroscopic devices, like utilisation of extremely long, linear detection arrays or strong [[defocus]] or other [[Aberration in optical systems|aberrations]] and makes the use of readily available 2D-detection arrays feasible, which amenorgues measurement times and improves efficiency.