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Scattering phenomenon

Phosphorescence Delayed fluorescence Thermal deactivation from T i [Pg.60]

Referring to the basic equations expressing the interaction between the radiation field and the molecular system, one can identify the existence of an intermediate state i) and a final state f) as a specific feature of scattering. The transition rate of the Raman scattering, WRaman, can be derived from Eqs. (1.113) and (1.114) in a way similar to that described in Section 1.4.2 for the case of the absorption and emission of light.I3) The derivations yield Eq. (1.158)  [Pg.62]

This quantity plays an important role in other multi-photon processes, such as two-photon absorption, second harmonic generation and hyper-Raman scattering as three-photon processes, and coherent anti-Stokes Raman scattering (CARS), a four-photon process (Table 1.5). The two-photon absorption can be treated theoretically from Eq. (1.115) in the same way as the Raman scattering process discussed above. Thus, the transition rate for two-photon absorption is given by Eq. (1.161). [Pg.62]

The relationship between second harmonic generation (SHG) and hyper-Raman scattering is similar to the relation between Rayleigh and Raman scatterings, in the case of two-photon [Pg.62]

Photophysical chemistry focuses primarily on the theory of the molecular system, although, strictly speaking, light absorption and emission processes are related to the interactions of the radiation field with the molecular system. Scattering processes are typical phenomena which are mainly concerned with the interaction of the radiation field with molecular systems. [Pg.63]


All scattering phenomena (light, x-rays and neutrons) can be interpreted in tenns of this equation (B1.9.5). [Pg.1387]

Chemistry students are familiar with spectrophotometry, the qualitative and quantitative uses of which are widespread in contemporary chemistry. The various features of absorption spectra are due to the absorption of radiation to promote a particle from one quantized energy state to another. The scattering phenomena we discuss in this chapter are of totally different origin classical not quantum physics. However, because of the relatively greater familiarity of absorption spectra, a comparison between absorption and scattering is an appropriate place to begin our discussion. [Pg.660]

Matrix absorption, secondary fluorescence and scattering phenomena limit sensitivity and precision in many cases, especially with dense matrices. The sensitivity falls off with atomic number elements with Z < 15 are particularly difficult to analyse. Analysis is characteristic of surface layers (5-500 pm depth) only for a solid specimen. Instruments are often large, complicated and costly. [Pg.336]

Table II lists several physical properties of various phosphors as compared to those for an ideal phosphor. The refractive index should be fairly low so that in a polymeric system (polymer Rl 1.5) the number of scattering phenomena are decreased. In this respect, BaFCI Eu is best. To reduce structure mottle and improve phosphor packing, spherical or polyhedral shaped particles are most desireable. Further, to improve phosphor packing, narrow particle distributions are best. Table II lists several physical properties of various phosphors as compared to those for an ideal phosphor. The refractive index should be fairly low so that in a polymeric system (polymer Rl 1.5) the number of scattering phenomena are decreased. In this respect, BaFCI Eu is best. To reduce structure mottle and improve phosphor packing, spherical or polyhedral shaped particles are most desireable. Further, to improve phosphor packing, narrow particle distributions are best.
It is noteworthy that for investigating pc-Ag electrodes, various surface spectroscopic methods have been utilized recently. A majority of the relevant papers are focused on the Raman scattering phenomena, mainly on the surface-enhanced Raman scattering (SERS) and related methods. One should emphasize that silver was one of the few noble metals for which the SERS response was observed, provided that the surface was previously activated by electrochemical or other means... [Pg.915]

This behavior is not observed uniquely when the angle between the two beams is 90° rather, the intensity of the reflected beam varies continuously with the angle. At 90°, however, the polarization effect is most pronounced. We shall see that some scattering phenomena also show an angular dependence, as well as the fact that scattered light displays maximum polarization at 90°. [Pg.199]

No pure compound with a peak at 375 m/j has been found to date, but occurrence of this peak certainly suggests that the compound responsible is related to the furfurals. An optical relationship also exists. When the colorant index is plotted against the frequency, the two peaks of 5-(hy-droxymethyl)-2-furaldehyde are found at 1305 and 1055 fresnels (sec.-1 X 1012). The peak of the unknown is at 805 fresnels, which is an exact, harmonic difference. The next harmonic would be at 555 fresnels or 540 m/j, in the general region in which the minima are found. The harmonic possible at 540 m/i is, unfortunately, in the region where light-scattering phenomena must also receive consideration. [Pg.282]

At energies above the edge, core electrons are excited to continuum states, and the spectrum becomes dominated by scattering phenomena, similarly as in EXAFS. Flence, in a qualitative sense, the shape of the XANES spectrum depends straightforwardly on the states that are available to the excited electron. These depend on several factors, such as the coordination of the atom (octahedral, tetrahedral, etc.), its mode of bonding, oxidation state, the density of states in the electron band, etc., which give XANES its great chemical sensitivity. [Pg.174]

Molecular beam scattering experiments provide direct and detailed information about the repulsive part of the interaction potential between the colliding particles. With such scattering data available, detailed studies of the short and intermediate-range parts of the potential energy surfaces can readily be made, provided that accurate theoretical methods, e.g. quantum close-coupling approach, are used to describe the scattering phenomena. [Pg.92]

The OCT has recently been extended to cover many orbital effects in the chemical bond and reactivity phenomena [38, 68-70]. The orbital communications have also been used to study the bridge bond order components [71, 72] and the multiple probability scattering phenomena in the framework of the probability-amplitude channel [73]. The implicit bond-dependency origins of the indirect (bridge) interactions between atomic orbitals in molecules have also been investigated [74],... [Pg.45]


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See also in sourсe #XX -- [ Pg.121 , Pg.122 , Pg.123 , Pg.124 , Pg.125 , Pg.126 ]

See also in sourсe #XX -- [ Pg.205 , Pg.213 ]




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Atmospheric Scattering Phenomena

Object scattering phenomenon

Scattering phenomena electromagnetic waves

Surface phenomena atom scattering

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