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Particle scattering process

Because of the existence of two-particle bound states the three-particle scattering states split into channels that means, we have to take into account scattering processes between free particles and bound pairs. To study the effect of composite particle scattering processes, we pay atten-... [Pg.199]

It is interesting to note that the processes (4.74) describe approximately only three-particle scattering processes. This follows from the fact that the integration over pb may be carried out in (4.71) if we take into account the approximation (4.68) and use only the first contribution of (4.72). The first contribution of Eq. (4.71) then reads... [Pg.245]

Figure Bl.24.4. Energy loss components for a projectile that scatters from depth t. The particle loses energy A E- via inelastic collisions with electrons along the inward path. There is energy loss A E in the elastic scattering process at depth t. There is energy lost to melastic collisions A along the outward path. For an incident energy Eq the energy of tlie exiting particle is = q - A iv - AE - A E. ... Figure Bl.24.4. Energy loss components for a projectile that scatters from depth t. The particle loses energy A E- via inelastic collisions with electrons along the inward path. There is energy loss A E in the elastic scattering process at depth t. There is energy lost to melastic collisions A along the outward path. For an incident energy Eq the energy of tlie exiting particle is = q - A iv - AE - A E. ...
Light-scattering processes involve the interaction of light with gases or particles in such a manner that the direction or frequency of the light is altered. Absorption processes occur when the electromagnetic radiation interacts with gases or particles and is transferred internally to the gas or particle. [Pg.138]

The formulation of the theory outlined above is particularly well-suited for the description of scattering processes, i.e., experiments consisting of the preparation of a number of physical, free noninteracting particles at t — oo, allowing these particles to interact (with one another and/or any external field present), and finally measuring the state of these particles and whatever other particles are present at time t = + co when they once again move freely. The infinite time involved... [Pg.586]

Fig. 22. The diagrams contributing to electrophoresis and the definition of lithe box. The reason why we only retain this class of terms is that we want to allow long-range propagation by the fluid— as shown in Fig. 21—which is clearly impossible if ions a and fi overlap in the box, because this would correspond to multiple scattering processes on particles a and fi. Fig. 22. The diagrams contributing to electrophoresis and the definition of lithe box. The reason why we only retain this class of terms is that we want to allow long-range propagation by the fluid— as shown in Fig. 21—which is clearly impossible if ions a and fi overlap in the box, because this would correspond to multiple scattering processes on particles a and fi.
Particles of a size of less than 2 turn are of particular interest in Process Engineering because of their large specific surface and colloidal properties, as discussed in Section 5.2. The diffusive velocities of such particles are significant in comparison with their settling velocities. Provided that the particles scatter light, dynamic light scattering techniques, such as photon correlation spectroscopy (PCS), may be used to provide information about particle diffusion. [Pg.9]

Each incident photon is treated as independent particle whose walk is randomized according to Eq. (8.3). The mean directional change in a scattering process is weighted by the anisotropy parameter g... [Pg.236]

For most scattering processes the relaxation times will depend on particle energy. Thus, we must average Eqs. (Alla) and (A1 lb) over energy. To simplify the notation we will write... [Pg.131]

The complete balance of the upturn by the polydispersity is only obtained for random branching processes. Often the reaction is impeded by serious constraints, or the primary chains before cross-linking are monodisperse. Then the resultant final molecular-weight distribution is narrower than in the random case, and the characteristic upturn as a result of branching, develops again. A strange coincidence in behavior is observed with star-molecules, where the rays are polydisperse, and with the ABC-type polycondensates. In both cases the particle-scattering factors can be expressed as ... [Pg.63]

BACKSCATTERING. The deflection of particles or of radiation by scattering processes through angles greater than 90° with respect to the original direction of motion. [Pg.167]

The technique for investigating scattering processes in crossed-beam experiments is well developed. For example, elastic scattering experiments with neutral particles at thermal energies are well understood,85 and the techniques for producing molecular and alkali atom beams and to detect them and interpret their kinematics has been reviewed on several occasions.86, 87. The new aspect of the present work is the technique for... [Pg.358]

Even the approximation (3.38) for 1234 contains, in a system supporting two-particle bound states, a large variety of scattering processes between subclusters. Among these possibilities, we consider only the scattering between the two (isolated) bound states (12) and (34). This means that... [Pg.207]

The Mpller operators of the last contribution, fl 123 4, describe scattering processes, in which particle 4 is asymptotically free. Thus, this last contribution vanishes. [Pg.209]

By that procedure, an additional factor V l appears in the equation of motion of pep [Eq. (4.29)]. This factor leads to the fact that the four-particle processes accounted for in this manner are not real and may vanish in the thermodynamic limit. At least this is true for four-particle scattering states. However, in the limiting case that we have only two-particle bound states, that is, the neutral gas, we can obtain a kinetic equation for the atoms if we use the special definition of the distribution function of the atoms (4.17) and (4.24). Using the ideas just outlined, the kinetic equation (4.62) was obtained. [Pg.242]


See other pages where Particle scattering process is mentioned: [Pg.957]    [Pg.959]    [Pg.1625]    [Pg.109]    [Pg.142]    [Pg.489]    [Pg.57]    [Pg.959]    [Pg.332]    [Pg.190]    [Pg.186]    [Pg.217]    [Pg.53]    [Pg.213]    [Pg.347]    [Pg.519]    [Pg.532]    [Pg.536]    [Pg.210]    [Pg.184]    [Pg.32]    [Pg.56]    [Pg.413]    [Pg.284]    [Pg.126]    [Pg.490]    [Pg.152]    [Pg.15]    [Pg.11]    [Pg.515]    [Pg.386]    [Pg.525]    [Pg.115]   
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