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Solid matrices at low temperature

2 x 10 5 M. Excitation wavelength 329.2 nm (adapted from Wehry and Mamantov, 1981). [Pg.69]

In argon or nitrogen matrices, the spectral resolution (bandwidth 100 cm-1) is not as high as in Shpol skii frozen solutions (bandwidth x 10 cm-1 or less). In the case of complex mixtures requiring high resolution, it is thus preferable to use Shpol skii solvents (n-alkanes and n-perfluoroalkanes). [Pg.70]

Site-selection spectroscopy Maximum selectivity in frozen solutions or vapor-deposited matrices is achieved by using exciting light whose bandwidth (0.01-0.1 cm-1) is less than that of the inhomogeneously broadened absorption band. Lasers are optimal in this respect. The spectral bandwidths can then be minimized by selective excitation only of those fluorophores that are located in very similar matrix sites. The temperature should be very low (5 K or less). The techniques based on this principle are called in the literature site-selection spectroscopy, fluorescence line narrowing or energy-selection spectroscopy. The solvent (3-methylpentane, ethanol-methanol mixtures, EPA (mixture of ethanol, isopentane and diethyl ether)) should form a clear glass in order to avoid distortion of the spectrum by scatter from cracks. [Pg.70]

Various compounds have been analyzed by site-selection spectroscopy. An interesting application is the identification of loci of damage in DNA resulting from reactions with carcinogens such as polycyclic aromatic hydrocarbons. [Pg.70]


A final note must be made about a common problem that has plagued many kinetic treatments of reactive intermediate chemistry at low temperatures. Most observations of QMT in reactive intermediates have been in solid matrices at cryogenic temperatures. Routinely, reactive intermediates are prepared for spectroscopy by photolyses of precursors imbedded in glassy organic or noble gas (or N2) solids. The low temperatures and inert surroundings generally inhibit inter- and intramolecular reactions sufficiently to allow spectroscopic measurements on conventional and convenient timescales. It is under such conditions, where overbarrier reactions are diminished, that QMT effects become most pronounced. [Pg.422]

Ono and Ware"" have measured the absorption, emission, and excitation spectra, the fluorescence decay times, and the quantum yields of a series of substituted diphenylmethylenes in rigid matrices at low temperatures. Acean-thrylene shows S2- So emission in hexane with a yield of 0.017 and lifetime of 4.3 ns. The low-temperature fluorescence spectra of bis-2-naphthyl-alkanes and their derivatives have been studied. Excimer formation is an activated process. The fluorescence and absorption spectra of 1,1-diphenyl-ethylenes have been analysed in some detail by Gustav and Bolke. " The S — Si transitions in trans isomers of phenylnaphthylethylenes have been assigned by picosecond absorption spectroscopy. Effects of solvent viscosity and the role of conformers in the mechanism of isomerization are elucidated. The production of non-equilibrium conformer concentrations in glassy solutions of diarylethylenes at 77 K due to restrictions imposed by the solid matrix has also been reported. Free jet excitation and emission spectra of diphenyl-butadiene show clearly the lowest excited Ag state and give a lifetime of 52.8 ns for 0-0 excitation.Electric field-induced charges in the optical... [Pg.13]

The simplest compound of the type RN=NR, di-imide, has been identified in the mass spectrometer among the solid products of decomposition of N2H4 by an electrodeless electrical discharge at 85°K. Both isomers have been identified (i.r.) in inert matrices at low temperatures (as also has imidogen, NH ), and the structure (a) has been assigned to the cis (planar) isomer... [Pg.647]

The sol-gel method allows the preparation of transparent, solid, and porous inorganic matrices at low temperatures, and the incorporation of organic molecules in its porosity [22,14]. The method involves reactions of hydrolysis and condensation of silicon aUcoxides (Figure 20.3) to produce a three-dimensional (3-D), amorphous, porous, and stable silica network. [Pg.449]

The co-condensation at low temperature of a metal vapor (commonly produced by resistance or electron-beam heating of metals) with a vapor of weakly stabilizing organic ligands (such as -pentane, toluene, tetrahydrofu-ran, acetone, or acetonitrile), using commercially available reactors, affords solid matrices, where reactions between the ligand molecules and metal atoms can take place (Scheme 1(A) Figure 1) [5]. [Pg.437]

Electron spin resonance (ESR) spectroscopy is of application to organic species containing unpaired electrons radicals, radical ions and triplet states, and is much more sensitive than NMR it is an extremely powerful tool in the field of radical chemistry (see Chapter 10). Highly unstable radicals can be generated in situ or, if necessary, trapped into solid matrices at very low temperatures. Examples of the application of this techniques include study of the formation of radical cations of methoxylated benzenes by reaction with different strong oxidants in aqueous solution [45], and the study of the photodissociation of N-trityl-anilines [46],... [Pg.71]

This section will be fairly brief because silabenzene and its congeners are unstable under normal conditions, and can be studied only at low temperatures or by trapping in solid matrices. Only when Tokitoh and coworkers introduced bulky and effective steric protecting groups such as tris[bis(trimethylsilyl)methyl]phenyl or Tbt groups was it possible to obtain kinetic stabilization and study silabenzene and germabenzene derivatives as stable crystalline compounds under normal conditions [218-221],... [Pg.230]

On the other hand, difficulty has been found in detecting the reaction intermediates using ESR spectroscopy. Initial studies39 with aryl halides using this technique at low temperature in solid matrices identified the n and a radical-anions of Phi. Dissociation of the radical anion (Phi)- to phenyl radical and iodide anion was also observed. These studies therefore provided evidence for the first two steps in the aromatic S l mechanism. [Pg.1400]

Z- E isomerization yield is nearly temperature-independent (Figure 1.10) or increases at low temperature, with only a small difference for excitation to the two lowest-excited states. So obviously, the E —> Z photoisomerization— after irradiation to the (n,7C ) state as well as the Z —> E isomerization— proceeds even at low temperature and in frozen solvents. In solid matrices, fast and slowly isomerizing molecules are observed on it —> it excitation. The fast process has a quantum yield of < = 0.14 that is temperature independent down to 4 K. With strong lasers, photoisomerization in the E —> Z direction have been exploited, even at 4 K in hole burning experiments. Thus, azobenzene photoisomerization cannot be frozen out. [Pg.23]

Because of the long radiative lifetime of the lowest triplet state, most phosphorescence in fluid solutions is obviated by collisional quenching, especially by dissolved molecular oxygen. Phosphorescence, when it occurs, is usually observed at low temperatures (e.g., that of liquid nitrogen) in rigid matrices where it may demonstrate high quantum yields. In the past three decades, much interest has been focused on phosphorescence at room temperature (RTP), which sometimes can be observed in samples adsorbed on solid substrates such as filter paper. Unfortunately, the quantum yields observed in room temperature phosphorescence are low, leading to poor analytical sensitivity, and the method has not enjoyed wide popularity. Phosphorescent measurements at low temperatures... [Pg.3388]

Figure 1. Excess internal energy (split in ion-dipole (fluio = flU o/V) and dipole-dipole (3un = SU fl/V) contributions) and chemical potential for a dipolar fluid inclusion in ionic matrices quenched at low temperature floe2/a — 1 (solid line and filled triangles) and high temperature floe2/a = 0.005 (dashed line and filled circles). The dotted lines correspond to the ion-dipole equilibrated mixture at fle2 /a = 1 for the corresponding charge densities. Curves denote ROZ results and symbols GCMC data[18]. Figure 1. Excess internal energy (split in ion-dipole (fluio = flU o/V) and dipole-dipole (3un = SU fl/V) contributions) and chemical potential for a dipolar fluid inclusion in ionic matrices quenched at low temperature floe2/a — 1 (solid line and filled triangles) and high temperature floe2/a = 0.005 (dashed line and filled circles). The dotted lines correspond to the ion-dipole equilibrated mixture at fle2 /a = 1 for the corresponding charge densities. Curves denote ROZ results and symbols GCMC data[18].

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Low temperature matrices

Solids temperature

Temperature at low

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