(spectroscopy) The use of spectrographs in conjunction with telescopes to obtain observational data on the velocities and physical conditions of astronomical objects.
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(spectroscopy) The use of spectrographs in conjunction with telescopes to obtain observational data on the velocities and physical conditions of astronomical objects.
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The use of spectroscopy (the analysis of light as a function of wavelength) as a tool for obtaining observational data on the chemical compositions, physical conditions, and radial velocities of astronomical objects. Astronomical applications of optical spectroscopy from ground-based observatories cover the electromagnetic spectrum from the near-ultraviolet (wavelengths around 0.3 micrometer) through the visible (0.4–0.7 μm) and into the near-infrared (2 μm). Space-based observatories extend spectroscopic observations from the far-ultraviolet (0.1 μm) to the far-infrared (100 μm). Work at shorter wavelengths (x-ray and gamma-ray spectroscopy) and longer wavelengths (submillimeter and radio wavelengths) requires techniques other than those discussed here. See also Gamma-ray astronomy; Radio astronomy; Satellite astronomy; Ultraviolet astronomy; X-ray astronomy.
Usually a spectrograph is fitted to a reflecting telescope, which serves as a light collector. The image of the celestial body being studied is focused on the spectrograph slit, which limits the region under study (thus improving the spectral resolution) and reducing the contribution by the night sky. The diverging light beam then passes from the slit to a collimator (either a lens or mirror). This produces parallel light, which is then dispersed by a diffraction grating or prism. The dispersed light enters a camera, which focuses the spectrum onto a detector, either a charge-coupled device (CCD) in the case of an optical spectrograph, or an electronic array sensitive to infrared light. See also Charge-coupled devices; Diffraction grating; Spectrograph; Spectroscopy.
It is often desirable to obtain spectroscopy of many of the objects within a telescope's field of view in a single exposure. A variety of methods are available to accomplish such surveys, including slitless spectroscopy, slitlet masks, and fiber-fed spectroscopy.
It is possible to take spectra of all of the brighter objects within the field of view by not using a spectrograph at all, but by combining a low-dispersing element directly with the telescope. For instance, an objective prism may be placed in front of the telescope, which is often a Schmidt camera. Slitless spectroscopy has been used for large stellar surveys. See also Astronomical catalogs.
In the technique of slitlet masks, a picture is usually taken of a region containing several astronomical objects of interest; the exact locations of these objects are determined, and small slits (slitlets) are then milled in the corresponding locations in a metal plate. This plate is substituted for the slit in a conventional spectrograph.
Rather than milling slitlets in a plate, holes may be drilled, which are then plugged with optical fibers. (Such an arrangement is often referred to as a plugboard.) The light is then transported via the fibers to a spectrograph mounted on an optical bench in a laboratorylike environment adjacent to the telescope. Alternatively, robotics may be used to position fibers in the focal plane; the fibers are then anchored to a metal plate via magnets. At the spectrograph, the fibers are arrayed in a line and act as the spectrograph slit. Hundreds of objects can be observed simultaneously, leading to very effective use of the telescope. See also Optical fibers.
Normal spectrographs employ diffraction gratings that are intended to be used in low orders (n = 1, 2, or 3), with colored glass filters used to prevent overlap of adjacent orders. Echelle spectrographs differ from conventional systems in that they employ gratings intended to be used in very high orders (n > 10), resulting in very high resolving power. Normally these orders would fall on top of one another, rendering the data useless. An echelle uses a second dispersal element, usually another grating but sometimes a prism, at right angles to the first, in order to separate the successive spectral strips from each other. A large range of wavelengths can be obtained in the format of nearly parallel segments, well suited for charge-coupled devices.
In integral field spectroscopy, a close-knit bundle of optical fibers is placed in the focal plane and is used to observe an extended astronomical object, such as a gaseous nebula or a galaxy. The light is transmitted via the fibers to a bench-mounted spectrograph. Although the fibers are in a linear array at the spectrograph, their locations in the focal plane are known, and sophisticated data reduction techniques allow the astronomer to reconstruct a spectral “image” of the object.
Fourier transform spectroscopy is used particularly in the near-infrared. Instead of being dispersed in a spectrograph, the light of a wide band of wavelengths is passed through a Michelson interferometer with variable spacing of its two apertures. The resulting interferogram, which is an electronic record of the interference signal produced by the interferometer as the separation of the apertures is varied, is converted into a record of intensity versus wavelength by a computer, and is of extremely high spectral resolution. See also Infrared spectroscopy; Interferometry.
The application of astronomical spectroscopy extends from solar system objects (the Sun, planets, and comets) to Milky Way objects (stars, including binary stars, ordinary novae, and cataclysmic variables; and gaseous nebulae, such as supernova remnants, H II regions, and planetary nebulae) and to distant galaxies and quasars.
| Wikipedia: Astronomical spectroscopy |
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Astronomical spectroscopy is the technique of spectroscopy used in astronomy. As spectroscopy is described in its own article, this article focuses on its use in astronomy. The object of study is the spectrum of electromagnetic radiation, including visible light, which radiates from stars and other celestial objects. Spectroscopy can be used to derive many properties of distant stars and galaxies, such as their chemical composition and also their motion, via the Doppler shift.
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Astronomical spectroscopy began with Isaac Newton's initial observations of the light of the Sun, dispersed by a prism. He saw a rainbow of colour, and may even have seen absorption lines. These dark bands which appear throughout the solar spectrum were first described in detail by Joseph von Fraunhofer. Most stellar spectra share these two dominant features of the Sun's spectrum: emission at all wavelengths across the optical spectrum (the continuum) with many discrete absorption lines superimposed on top.
Fraunhofer's original (1817) designations of absorption lines in the solar spectrum
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Fraunhofer and Angelo Secchi were among the pioneers of spectroscopy of the Sun and other stars. Secchi is particularly noted for classifying stars into spectral types, based on the number and strength of the absorption lines in their spectra. Later the origin of the spectral types was found to be related to the temperature of the surface of the star: particular absorption lines can be observed only for a certain range of temperatures; because only in that range are the involved atomic energy levels populated.
The absorption lines in stellar spectra can be used to determine the chemical composition of the star. Each element is responsible for a different set of absorption lines in the spectrum, at wavelengths which can be measured extremely accurately by laboratory experiments. Then, an absorption line at the given wavelength in a stellar spectrum shows that the element must be present. Of particular importance are the absorption lines of hydrogen (which is found in the atmosphere of nearly every star); the hydrogen lines within the visual spectrum are known as Balmer lines.
In 1868, Sir Norman Lockyer observed strong yellow lines in the solar spectrum which had never been seen in laboratory experiments. He deduced that they must be due to an unknown element, which he called helium, from the Greek helios (sun). Helium wasn't conclusively detected on earth until 25 years later.
Also in the 1860s, emission lines (particularly a green line) were observed in the coronal spectrum during solar eclipses that did not correspond to any known spectral lines. Again it was proposed that these were due to an unknown element, provisionally named coronium. It was not until the 1930s that it was discovered that these lines were due to highly ionised iron and nickel, the high ionisation being due to the extreme temperature of the solar corona.
In conjunction with atomic physics and models of stellar evolution, stellar spectroscopy is today used to determine a multitude of properties of stars: their distance, age, luminosity and rate of mass loss can all be estimated from spectral studies, and Doppler shift studies can uncover the presence of hidden companions such as black holes and exoplanets.
In the early days of telescopic astronomy, the word nebula was used to describe any fuzzy patch of light that didn't look like a star. Many of these, such as the Andromeda Nebula, had spectra that looked in many ways a lot like stellar spectra, and these turned out to be galaxies. Others, such as the Cat's Eye Nebula, had very different spectra. When William Huggins looked at the Cat's Eye, he found no continuous spectrum like that seen in the Sun, but just a few strong emission lines. These lines did not correspond to any known elements on earth, and so just as helium had been identified in the Sun, astronomers suggested that the lines were due to a new element, nebulium (occasionally nebulum or nephelium). The hypothetical nebulium that was invoked to account for certain bright lines in gaseous nebulae were shown by Ira Sprague Bowen in 1927 as due to doubly ionized oxygen at extremely low density. As Henry Norris Russell put it, "Nebulium has vanished into thin air." But nebulae are typically extremely rarefied, much less dense than the hardest vacuum ever produced on earth. In these conditions, atoms behave quite differently and lines can form which are suppressed at normal densities. These lines are known as forbidden lines, and are the strongest lines in most nebular spectra.
The spectra of galaxies look somewhat similar to stellar spectra, as they consist of the light from millions of stars combined. Galactic spectroscopy has led to many fundamental discoveries. Edwin Hubble discovered in the 1920s that, apart from the nearest ones (those in what is known as the Local Group), all galaxies are receding from the Earth. The further away a galaxy, the faster it is receding (see Hubble's Law). This was the first indication that the universe originated from a single point, in a Big Bang.
Doppler shift studies of clusters of galaxies by Fritz Zwicky found that most galaxies were moving much faster than seemed to be possible, from what was known about the mass of the cluster. Zwicky hypothesised that there must be a great deal of non-luminous matter in the galaxy clusters, which became known as dark matter.
In the 1950s, some strong radio sources were found to be associated with very dim objects that seemed to be very blue. These were named Quasi-stellar radio sources, or quasars. When the first spectrum of one of these objects was taken, it was something of a mystery, with absorption lines at wavelengths where none were expected. It was soon realised that what was being seen was a normal galactic spectrum, but highly redshifted. According to Hubble's Law, this implied that the quasar must be extremely distant, and therefore highly luminous. Quasars are now thought to be galaxies forming, with their extreme energy output being powered by super-massive black holes.
Planets and asteroids shine only by reflecting the light of their parent star. The reflected light contains absorption bands due to minerals in the rocks present for rocky bodies, or due to the elements and molecules present in the atmospheres of the Gas giants. Asteroids can be classified into three main types, according to their spectra: the C-types are made of carbonaceous material, S-types consist mainly of silicates, and M-types are 'metallic'. C- and S-type asteroids are the most common.
The spectra of comets consist of a reflected solar spectrum from the dusty clouds surrounding the comet, as well as emission lines from gaseous atoms and molecules excited by sunlight fluorescence and/or chemical reactions. Nearby comets can even be seen in X-ray as solar wind ions flying to the coma are neutralized, and cometary X-ray spectra therefore reflect the state of the solar wind rather than that of the comet. Many organic chemicals are known to exist in comets, and it has been suggested that cometary impacts provided the Earth with much of the water for its oceans and the chemicals necessary for the formation of life. It has even been suggested that life may have been brought to earth from interstellar space by comets (the Panspermia theory).
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| slitlet mask (spectroscopy) | |
| spectropyrheliometer (spectroscopy) | |
| Vesto Melvin Slipher (American astronomer) |
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