The following section describes a common technique for optimizing diffraction efficiencies. In general, diffraction efficiencies can be calculated with diffraction theory.Ī high diffraction efficiency for a particular diffraction order is essential for various applications.įor example, a pulse compressor setup should not waste more of the generated pulse energy than is unavoidable.Īlso, high throughput of a spectrometer, enabled by using one or more highly efficient gratings, leads to a high detection sensitivity or possibly to reduced demands on the probe illumination, which is particularly important for battery-powered instruments. This depends on the shape of the wavelength-dependent phase changes, and thus on the detailed properties of the grating grooves. In other words, the diffraction efficiency for certain diffraction orders is of interest. Unlike a simple prism, a diffraction grating generally produces multiple output beams according to different diffraction orders.Īn important question is how the output power is distributed over the different diffraction orders. Distribution of the Output Power on the Diffraction Orders The number of orders increases for shorter wavelengths and larger grating periods. Figure 3:Ĭolor-coded number of non-zero diffraction orders as a function of the wavelength divided by the grating period.įigure 3 shows how the number of diffraction orders depends on the ratio of wavelength and grating period, and on the angle of incidence. The order m = 2, for example, is possible only for wavelengths below 560 nm.Īs the direction of each output beam – except for the zero-order beam – is wavelength-dependent, a diffraction grating can be used as a polychromator. The incident beam has fixed angle of 25° against the normal direction.įigure 2 shows in an example case of a grating with 800 lines per millimeter, how the output angles vary with wavelength.įor the zero-order output (pure reflection, m = 0), the angle is constant, whereas for the other orders it varies. Output angles of a reflective diffraction grating with 800 lines per millimeter as functions of the wavelength. The equations above may lead to values of sin θ out with a modulus larger than 1 in that case, the corresponding diffraction order is not possible.įigure 1 shows an example, where the diffraction orders −1 to +3 are possible. Note that different sign conventions may be used for the diffraction order, so that there may be a minus sign in front of that term. Note that there are also volume Bragg gratings, where the diffraction occurs inside the bulk material. This article treats mainly diffraction gratings where the diffraction occurs at or near the surface. However, there are also transmission gratings, where transmitted light obtains position-dependent phase changes, which may also result from a surface relief, or alternatively from a holographic ( interferometric) pattern. Most common are reflection gratings (or grating reflectors), where a reflecting surface has a periodic surface relief leading to position-dependent phase changes. It contains a periodic structure, which causes spatially varying optical amplitude and/or phase changes. Diffraction grating how to#How to cite the article suggest additional literatureĪ diffraction grating is an optical device exploiting the phenomenon of diffraction, i.e., an kind of diffractive optics. the wavelength-dependent beam path in a single-pass configuration or within a laser resonator.ĭefinition: optical components containing a periodic structure which diffracts light Diffraction grating software#The software RP Resonator also works with gratings.Find out e.g. Analyzing Beam Pathes Containing Gratings Using our ad package, you can display your logo and further below your product description.
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