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Excitation by photons

As we have seen, the electron is the easiest probe to make surface sensitive. For that reason, a number of hybrid teclmiques have been designed that combine the virtues of electrons and of other probes. In particular, electrons and photons (x-rays) have been used together in teclmiques like PD [10] and SEXAFS (or EXAFS, which is the high-energy limit of XAES) [2, Hj. Both of these rely on diffraction by electrons, which have been excited by photons. In the case of PD, the electrons themselves are detected after emission out of the surface, limiting the depth of sampling to that given by the electron mean free path. [Pg.1756]

A further technique exists for the determination of triplet energy levels. This technique, called electron impact spectroscopy, involves the use of inelastic scattering of low-energy electrons by collision with molecules. The inelastic collisions of the electrons with the molecules result in transfer of the electron energy to the molecule and the consequent excitation of the latter. Unlike electronic excitation by photons, excitation by electron impact is subject to no spin selection rule. Thus transitions that are spin and/or orbitally forbidden for photon excitation are totally allowed for electron impact excitation. [Pg.117]

Figure 12.7 The photosynthetic unit, in which an antenna chlorophyll molecule is excited by photon absorption and the energy is transferred to the chlorophyll dimer at the reaction centre... Figure 12.7 The photosynthetic unit, in which an antenna chlorophyll molecule is excited by photon absorption and the energy is transferred to the chlorophyll dimer at the reaction centre...
The activation step can alternatively be performed without gas by means of infrared multiphoton dissociation (IRMPD) or electron capture dissociation (BCD) (Chap. 2.12.2). Both IRMPD and BCD, solely require storage of the ions during their excitation by photons or electrons, respectively. It is one of the most charming properties of FT-ICR-MS/MS that even the accurate mass of the fragment ions can be determined. [216,217]... [Pg.172]

Jacoby et al. (1994) studied the photocatalytic reaction of gaseous trichloroethylene in air in contact with UV-irradiated titanium dioxide catalyst. The UV radiation was kept less than the maximum wavelength so that the catalyst could be excited by photons, i.e., X <356 nm. Two reaction pathways were proposed. The first pathway includes the formation of the intermediate dichloroacetyl chloride. This compound has a very short residence time and is quickly converted to the following compounds phosgene, carbon dioxide, carbon monoxide, carbon dioxide, and hydrogen chloride. The second pathway involves the formation of the final products without the formation of the intermediate. [Pg.1096]

AFS involves the emission of photons from an atomic vapour that has been excited by photon absorption. For low absorbance signals (and thus for low... [Pg.8]

Certain compounds, whether present in solution or in solid state (as molecular or ionic crystals) emit light when they are excited by photons in the visible or near ultraviolet domain of the spectrum. This phenomenon, called luminescence, is the basis of fluorimetry, a very selective and sensitive analysis technique. The corresponding measurements are made with fluorimeters or spectrofluorimeters and, for chromatographic applications, with fluorescence detectors. [Pg.221]

Excitation by Photons. The dependence of the absorptivity of a phosphor upon the photon energy is given by the absorption spectrum. This can be divided into various regions such as basic lattice absorption, edge absorption, and defect absorption [5.307]. [Pg.237]

Direct verification of DR-mechanism of DIET was provided [21] by combining the state-selective photoexcitation of the sample and the controlled thermally induced release of electrons from electron traps (Fig.9a). In RGS, after electron-hole pair creation at selective excitation by photons with energies E>Eg, the hole may survive and be self-trapped if the electron is captured by any kind of traps [32], In solid Ar at T>2 K the main part of electron traps is not active [12], the electron-hole recombination occurs before self-trapping the holes, and, therefore, the concentration of W-band emitting centers decreases (Fig.9a). On the contrary, the heating... [Pg.54]

It would follow that quantums of one energy cannot interfere with quantums of another energy. Furthermore, the appearance of horizontal parts in the Arrhenius plot with activation energy zero were not possible in the light, because the dark reaction occuring simultaneously on the sites not excited by photon absorption ought to be observed in the light, too. [Pg.142]

The Rate Equations. As illustrated in Figure 1, molecules are excited by photon absorption in the process... [Pg.62]

Measuring An in a spectral region were Ak is much smaller. Such nonlinearities are referred to as non-resonant (associated with virtual states), being excited by photon energies far away from any electronic transition. These nonlinearities can be exploited in photonic devices for full optical signal processing, in which optical losses due to real absorption are kept low [31,45-52,78]. [Pg.72]

Two other ion activation methods were developed to replace the gas molecules as targets by laser beams (photodissociation or infrared multiphoton dissociation IRMPD) or by electron beams (electron capture dissociation ECD). These two methods can be applied to ions that are trapped during their excitations by photons or electrons, respectively. Thus, they are most often used with ion trap or ICR analysers because the residence time and the interaction time are longer. [Pg.200]

Nomenclature and Spectral Presentation in Electron Spectroscopy Resulting from Excitation by Photons, Pure Appl. Chem. 45 (1976) 221-224. [Pg.137]

In catalyzed photolysis either the catalyst molecule (Fig. 5-11, situation B) or the substrate molecule (Fig. 5-11, situation C), or both, are in an electronically excited state during the catalytic step. The electronically excited catalyst molecule is produced via photon absorption by a nominal catalyst (Fig. 5-11, situation B). The reaction of substrate to product is catalytic with, respect to the concentration of the electronically excited catalyst species. It is non-catalytic in photons and therefore, continuous irradiation is required to maintain the catalytic cycle. The quantum yield of product formation Product is equal to or less than unity. Titanium dioxide photocatalysis is the most widely applied example of this type, with Ti02 representing the nominal catalyst that must be electronically excited by photon absorption with formation of the electron hole pair Ti02 (hvb + cb), being the active catalytic species (cf Fig. 3-17 and Fig. 5-9, reaction 1). The oxidation of substrates by the combination of UV/VIS radiation and an appropriate photocatalyst is often called photocatalytic oxidation (PCO). [Pg.121]

Ions are formed by the action of particle beams, decomposition of molecules excited by photons, donor-acceptor interactions of suitable compounds and by the effects of an electric current on solutions of supporting electroly-tes. Some special polymerization processes can be initiated by anions and cations generated in this way. The practical importance of all the enumerated methods is so far not large. Nevertheless, these processes continue to be the subject of intense study. A short description of the most interesting of these methods is contained in Sects. 5 and 6.1. Polymerization-initiating anions can even be formed from cations (see Chap. 4, Sect. 5). [Pg.118]

Fluorescence Radiation produced by an atom or a molecule that has been excited by photons to a singlet excited state. Fluorescence bands Groups of fluorescence lines that originate from the same excited electronic state. [Pg.1109]

P E, hv) is the distribution of photoelectron energy, E, excited by photon of energy, hv, T E) is the transmission function and D E) is the escape function. Both T E) and D(E) are smoothly varying functions. Therefore the structures in the observed intensities are almost entirely determined by P E, hv). The photoelectron energy distribution function is given by. [Pg.313]

Depending on the excitation method used, luminescence techniques are divided into photoluminescence excited by photons, cathodoluminescence generated under the action of cathode rays, X-ray luminescence excited by X-rays, candoluminescence generated under the action of heat, and sonoluminescence excited by ultrasound. Emission generated under the action of a stream of ions from alkali metals in vaccum is called ionoluminescence radiation which atoms emit on optical excitation in plasma is known as atomic fluorescence chemiluminescence is the emission of radiation generated by the energy of chemical reactions, it does not require an external excitation source. The excitation source needed in each particular case is chosen on the basis of this classification. [Pg.55]

Photo- ionization (PID) Samples are ionized by excitation by photons from a UV lamp 1-10 pg 10 More sensitive to aromatics than to aUphatics... [Pg.84]


See other pages where Excitation by photons is mentioned: [Pg.758]    [Pg.271]    [Pg.66]    [Pg.373]    [Pg.51]    [Pg.119]    [Pg.133]    [Pg.16]    [Pg.159]    [Pg.160]    [Pg.130]    [Pg.200]    [Pg.184]    [Pg.105]    [Pg.139]    [Pg.3786]    [Pg.61]    [Pg.287]    [Pg.195]    [Pg.87]    [Pg.241]    [Pg.606]    [Pg.388]   
See also in sourсe #XX -- [ Pg.89 , Pg.143 ]

See also in sourсe #XX -- [ Pg.89 , Pg.143 ]




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