diffraction grating(redirected from Reflection Grating)
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An optical device consisting of an assembly of narrow slits or grooves, which by diffracting light produces a large number of beams which can interfere in such a way as to produce spectra. Since the angles at which constructive interference patterns are produced by a grating depend on the lengths of the waves being diffracted, the waves of various lengths in a beam of light striking the grating will be separated into a number of spectra, produced in various orders of interference on either side of an undeviated central image. By controlling the shape and size of the diffracting grooves when producing a grating and by illuminating the grating at suitable angles, a beam of light can be thrown into a single spectrum whose purity and brightness may exceed that produced by a prism. Gratings can now be made with much larger apertures than prisms, and in such form that they waste less light and give higher intrinsic dispersion and resolving power. See Diffraction
Transmission gratings consist of a large number of narrow transparent and opaque slits alternating side by side in regular order and with uniform separation, through which a beam of light will appear as a series of spectra in various orders of interference. Reflection gratings, either plane or concave, are used in most spectrographs. Such a grating may consist of an original ruling or of a metal-coated replica from an original. Large grating replicas can now be made which are practically indistinguishable in performance or permanence from an original.
Gratings are engraved by highly precise ruling engines, which use a diamond tool to press into a highly polished mirror surface a series of many thousands of fine shallow burnished grooves. If a grating is to give resolution approaching the theoretical limit, its grooves must be ruled straight, parallel, and equally spaced to within a few tenths of the shortest incident wavelength. Scattered light and false images may arise from local spacing error and groove shape variations of only a few hundredths of the diffracted wavelength.
A grating spectroscope usually consists of a slit, a lens or mirror to collimate the light sent through the slit into a parallel beam, a transmission or reflection grating to disperse the light, a lens or mirror to focus the light into spectrum lines (which are monochromatic images of the slit in the light of each wavelength passing through it), and an eyepiece for viewing the spectrum. If a camera is substituted for the telescope, the instrument becomes a grating spectrograph. If a photoelectric cell, a thermocouple, or other radiation-detecting device is used instead of a camera or telescope, the device becomes a grating spectrometer. See Infrared spectroscopy
diffraction gratingA device usually incorporated into a spectrograph and employed in the production and study of spectra. Its action depends on the diffraction of light or other radiation by a very large number of very close and exactly equidistant parallel linear grooves. The grooves are produced by ruling very fine closely spaced scratches on glass or polished metal, forming either a transmission grating in the first case or a reflection grating in the second. These ruled gratings are very costly, and replica gratings – accurate plastic casts of ruled gratings – are usually used instead. Reflection gratings can be plane or concave; the latter can act as a focusing element for incident radiation, which would otherwise be partly absorbed if a lens were employed.
The diffracted radiation, once focused, produces a series of sharp spectral lines for each resolvable wavelength present in the incident beam. For a plane wave of a single wavelength λ, incident on a transmission grating at angle i , the successive wave trains passing through the grooves will travel different pathlengths. If the path difference between two adjacent grooves is a whole number of wavelengths, the wave trains will be brought to a focus as a bright image of the radiation source at a particular angle of refraction, d (see illustration), where
s is the spacing between adjacent grooves and n is an integer. Bright images will in fact be produced for each of the angles d corresponding to n = 1, 2, 3… These numbers denote the orders of the image. If, for a particular order, d is made equal to i , then
an optical device that consists of a large number of parallel, equidistant, and identically shaped lines marked on a flat or concave optical surface. A diffraction grating is a periodic structure: the lines, whose shape is definite and constant for a given grating, repeat over a strictly identical interval d, known as the period of the grating (see Figure 1). Diffraction of light occurs in a diffraction grating.
The main property of a diffraction grating is the ability to resolve an incident beam of light by wavelengths (that is, into a spectrum); this property is used in spectral apparatus. A plane diffraction grating has lines marked on a plane surface; a concave grating has lines marked on a concave, usually spherical, surface. Diffraction gratings may also be classified as reflective of transmission. The lines of reflective gratings are marked on a mirror surface (usually metal), and observations are made in reflected light. The lines of transmission gratings are marked on the surface of a transparent plate (usually made of glass), or they may be narrow slits in an opaque screen; observations are made in the transmitted light. Reflective diffraction gratings are usually used in modern spectral instruments.
The principle of operation of a diffraction grating is most clearly shown by a transmission grating, when a monochromatic, parallel beam of light of wavelength λ is incident on the diffraction grating at an angle α. The diffraction grating consists of slits of width b separated by opaque intervals; interference of the light emanating from the individual slits occurs. As a result, after focusing on a screen, the location of the maximums (Figure 1) may be determined by the equation d (sin α + sin β) = mλ, where β is the angle between the direction normal to the grating and the direction of propagation of the beam (the diffraction angle); the integer m = 0, ±1, ±2, ±3, … is equal to the number of wavelengths by which a wave from some element of a given slit of the diffraction grating lags behind or leads the wave emanating from the same element of an adjacent slit. Monochromatic beams corresponding to the different values of m are called spectral orders, and the images of the entrance slits projected by the beams are called spectral lines. All orders that correspond to the positive and negative values of m are located symmetrically with respect to the zero order. The spectral lines become narrower and sharper as the number of slits is increased. If the radiation incident on a diffraction grating has a complex spectral composition, each wavelength will have its own set of spectral lines, and consequently, the radiation will be resolved into spectra according to the number of possible values for m. The relative intensity of the lines is determined by the energy distribution function for a particular slit.
The two main characteristics of a diffraction grating are its angular dispersion and its resolving power. Angular dispersion, which determines the angular width of the spectrum, depends on the difference ratio of diffraction angles for two wavelengths:
Thus, the angular width of the spectrum varies approximately proportional to the order number of the spectrum. The resolving power R is defined by the ratio of the wavelength to the smallest wavelength interval that still can by separated by the grating:
where N is the number of slits in the diffraction grating and W is the width of the hatched surface. The resolving power for given angles can be increased only by increasing the width of the grating.
Diffraction gratings used for work in various regions of the spectrum differ with respect to the frequency and shape of the lines and to the dimensions, shape, and material of the surface. Diffraction gratings for the ultraviolet and visible regions typically have 300-1,200 lines per mm. In such diffraction gratings the lines are made in a layer of aluminum deposited on a glass surface by vacuum evaporation. Diffraction gratings for the vacuum ultraviolet region are usually made on glass surfaces. Gratings marked on a concave (usually spherical) surface, which is capable of focusing the spectrum, are indispensable for this region. Diffraction gratings used in the infrared region are called echelettes; they have 300-0.3 lines per mm and are made from various soft metals.
Diffraction gratings are used not only in spectral instruments but also as optical sensors of linear and angular displacement (measuring diffraction gratings), as polarizers and filters of infrared radiation, and as beam splitters in interferometers. Diffraction gratings of all of the known types are manufactured in the USSR. The maximum number of lines per mm is 2,400, and the maximum dimensions of the hatched area are 300 × 300 mm.
REFERENCESLandsberg, G. S. Optika, 4th ed. Moscow, 1957. (Kurs obshchei fiziki, vol. 3.)
Tarasov, K. I. Spektral’nye pribory. Leningrad, 1968.
(See also references in DIFFRACTION OF LIGHT.)
F. M. GERASIMOV