(spectroscopy) A spectroscopic technique in which reactive species can be characterized by maintaining them in a very cold, inert environment while they are examined by an absorption, electron-spin resonance, or laser excitation spectroscope.
| Sci-Tech Dictionary: matrix isolation |
(spectroscopy) A spectroscopic technique in which reactive species can be characterized by maintaining them in a very cold, inert environment while they are examined by an absorption, electron-spin resonance, or laser excitation spectroscope.
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| Sci-Tech Encyclopedia: Matrix isolation |
A technique for providing a means of maintaining molecules at low temperature for spectroscopic study. This method is particularly well suited for preserving reactive species in a solid, inert environment. Elusive molecular fragments, such as free radicals that may be postulated as important controlling intermediates for chemical transformations used in industrial reactions, high-temperature molecules that are in equilibrium with solids at very high temperatures, and molecular ions that are produced in plasma discharges or by high-energy radiation all can be examined by using absorption (infrared, visible, and ultraviolet), electron-spin resonance, and laser-excitation spectroscopes.
The experimental apparatus for matrix isolation experiments is designed with the method of generating the molecular transient and performing the spectroscopy in mind. The illustration shows the cross section of a vacuum vessel used for absorption spectroscopic measurements. The matrix sample is introduced through the spray-on line; argon is the most widely used matrix gas, although neon, krypton, xenon, and nitrogen are also used. The reactive species can be generated in a number of ways: mercury-arc photolysis of a trapped precursor molecule through the quartz window, evaporation from a Knudsen cell in the heater, chemical reaction of atoms evaporated from the Knudsen cell with molecules deposited through the spray-on line, and vacuum-ultraviolet photolysis of molecules deposited from the spray-on line by radiation from discharge-excited atoms flowing through the tube. For laser excitation studies, the sample is deposited on a tilted copper wedge which is grazed by the laser beam, and light emitted or scattered at approximately 90° is examined by a spectrograph. In electronspin resonance studies, the sample is condensed on a sapphire rod that can be lowered into the necessary waveguide and magnet.

Vacuum-vessel base cross section for matrix photoionization experiments.
The matrix isolation technique enables spectroscopic data to be obtained for reactive molecular fragments, many of which cannot be studied in the gas phase.
| Wikipedia: Matrix isolation |
Matrix isolation is an experimental technique used in chemistry and physics which generally involves a material being trapped within an unreactive matrix. A host matrix is a continuous solid phase in which guest particles (atoms, molecules, ions, etc.) are embedded. The guest is said to be isolated within the host matrix. Initially the term matrix-isolation was used to describe the placing of a chemical species in any unreactive material, often polymers or resins, but more recently has referred specifically to gases in low-temperature solids. A typical matrix isolation experiment involves a guest sample being diluted in the gas phase with the host material, usually a noble gas or nitrogen. This mixture is then deposited on a cold window, often cooled to 10 kelvins or below. The sample may then be studied using various spectroscopic procedures.
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The transparent window, on to which the sample is deposited, is usually cooled using a compressed helium or similar refrigerator. Experiments must be performed under a high vacuum to prevent contaminates from unwanted gases freezing to the cold window. Lower temperatures are preferred, due to the improved rigidity and “glassiness” of the matrix material. Noble gases such as argon are used not just because of their unreactivity but also because of their broad optical transparency in the solid state. Mono-atomic gases have relatively simple face-centered cubic (fcc) crystal structure, which can make interpretations of the site occupancy and crystal-field splitting of the guest easier. In some cases a reactive material, for example, methane, hydrogen or ammonia, may be used as the host material so that the reaction of the host with the guest species may be studied.
Using the matrix isolation technique, short-lived, highly-reactive species such as radical ions and reaction intermediates may be observed and identified by spectroscopic means. For example, the solid noble gas krypton can be used to form an inert matrix within which a reactive F3- ion can sit in chemical isolation. A species may be created chemically before deposition, or after by photochemical means. The technique may be used to simulate a species in the gas phase without rotational and translational interference. The low temperatures also help to produce simpler spectra, since only the lower electronic and vibrational quantum states are populated.
Matrix isolation has its origins in the first half of the 20th century with the experiments by photo-chemists and physicists freezing samples in liquefied gases. The earliest isolation experiments involved the freezing of species in transparent, low temperature organic glasses. The modern matrix isolation technique was developed extensively during the 1950s, in particular by George C. Pimentel. He initially used higher-boiling inert gases like xenon and nitrogen as the host material, and is often said to be the "father of matrix isolation".
Dunkin, Iain R (1998). Matrix-Isolation Techniques - A Practical Approach. Oxford: Oxford University Press. ISBN 0-19-855863-5.
Daintith, John (senior editor) (2004). Oxford Dictionary of Chemistry. Oxford: Oxford University Press. ISBN 0-19-860918-3.
Ball, David W. , Zakya H. Kafafi, et al., A Bibliography of Matrix Isolation Spectroscopy, 1954-1985, Rice University Press, Houston, 1988
NIST Optical Technology Division [1]
IUPAC Compendium of Chemical Terminology (Second Edition), 1997 [2]
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