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Linear scattering

Experimentally accessible is D by means of scattering methods [144], The corresponding fractal analysis of scattering data is gaining special attractivity from its intriguing simplicity. In a double-logarithmic plot of I (s) v.v. s the fractal dimension is directly obtained from the slope of the linearized scattering curve. It follows from the theory of fractals that... [Pg.143]

Jauncey has recently described a corpuscular quantum theory of the scattering of polarized X-rays, in which a formula for the intensity of the scattering in any direction is derived. From this formula an expression for the linear scattering coefl cient per unit solid angle in any direction 4> may be obtained. In particular this linear scattering coefficient for the case where plane polarized X-rays are scattered in the plane of the electric vector of the primary X-rays is given by... [Pg.8]

The linear scattering coefficient of limestone dust in the air is 0.0002194 m . Over what distance will the intensity of a light beam diminish to 10 % of its initial value ... [Pg.472]

Quantitative application of Raman spectroscopy generally requires pretreatment to reduce background variance and often also includes the application of chemometric methods. The success of both steps depends on a high level of both abscissa and ordinate stability and linearity. Scattering intensity and the relative intensities of Raman lines within a spectrum depend on a variety of measurement conditions laser power, laser wavelength, spectral resolution, detector properties, and arrangement of the excitation and collection optics. [Pg.265]

Hyper-Raman light scattering is that, unlike linear scattering (see Section 3.2.5), two photons with the frequency nj participate in the inelastic collision with the particle B(J). As a result, a molecule in the different eneigy state and one photon with the energy /ii are formed... [Pg.87]

At this stage it may be desirable to compare resonance Raman spectroscopy with FT-Raman spectroscopy. FT-Raman spectroscopy allows vibrations that are not associated with the electronic chromophore to be observed. Additionally, FT-Raman spectroscopy exhibits linear scattering intensities that allow quantitative analysis. On the other hand, resonance Raman spectroscopy is much more sensitive than FT-Raman spectroscopy [28]. [Pg.231]

Fig. 2 shows the response of a C2 film system on a step wedge (wall thickness range 2. .. 18 mm) exposed with a X-ray tube at 160 kV. For the exposure withy-rays (Irl92 or Co60) corresponding linear relationships are obtained. From this linear relationship it is followed, that the influence of the scattered radiation and the energy dependence of the absorption coefficient can be considered by an effective absorption coefficientPcff in equation (1). [Pg.562]

Let us consider the scheme showed in Fig. I to calculate the field scattered by a rough cylindrical surface (i.e. a wire). The wire is illuminated by a monochromatic, linearly polarized plane wave at an angle of incidence a with its axis of symmetry. The surface is described, in a system fixed to the wire, by p = h (cylindrical coordinates. We shall denote the incident wave vector lying on the x-z plane as kj and the emergent wave vector simply as k. [Pg.663]

Lefebvre, J.P., Progress in linear inverse scattering imaging NDE application of Ultrasonic Reflection Tomography, in Inverse Problem in Engineering Mechanies, pp 371-375, (A.A.Balkema/ Rotterdam rookfleld, 1994). [Pg.750]

The current frontiers for the subject of non-equilibrium thennodynamics are rich and active. Two areas dommate interest non-linear effects and molecular bioenergetics. The linearization step used in the near equilibrium regime is inappropriate far from equilibrium. Progress with a microscopic kinetic theory [38] for non-linear fluctuation phenomena has been made. Carefiil experiments [39] confinn this theory. Non-equilibrium long range correlations play an important role in some of the light scattering effects in fluids in far from equilibrium states [38, 39]. [Pg.713]

Radiation probes such as neutrons, x-rays and visible light are used to see the structure of physical systems tlirough elastic scattering experunents. Inelastic scattering experiments measure both the structural and dynamical correlations that exist in a physical system. For a system which is in thennodynamic equilibrium, the molecular dynamics create spatio-temporal correlations which are the manifestation of themial fluctuations around the equilibrium state. For a condensed phase system, dynamical correlations are intimately linked to its structure. For systems in equilibrium, linear response tiieory is an appropriate framework to use to inquire on the spatio-temporal correlations resulting from thennodynamic fluctuations. Appropriate response and correlation functions emerge naturally in this framework, and the role of theory is to understand these correlation fiinctions from first principles. This is the subject of section A3.3.2. [Pg.716]

In the next section we discuss linear hydrodynamics and its role in understanding the inelastic light scattering experiments from liquids, by calculating the density-density correlation fiinction,. Spp. [Pg.722]

Now let us return to the Kolm variational theory that was introduced in section A3.11.2.8. Here we demonstrate how equation (A3.11.46) may be evaluated using basis set expansions and linear algebra. This discussion will be restricted to scattering in one dimension, but generalization to multidimensional problems is very similar. [Pg.988]

Alexander M H and Manolopoulos D E 1987 A stable linear reference potential algorithm for solution of the quantum close-coupled equations in molecular scattering theory J. Chem. Phys. 86 2044-50... [Pg.1086]


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See also in sourсe #XX -- [ Pg.24 ]




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