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Calculation of scattering amplitudes

There are two characteristic difficulties of multichannel many-fermion problems. The first is that computational methods can of course directly address only a finite number of channels whereas the physical problem has an infinite number of discrete channels and the ionisation continuum. The second is that the electrons are identical so that the formulation in terms of one-electron states must be explicitly antisymmetric in the position (or momentum) and spin coordinates. [Pg.156]


Both integrals do not require assumption of periodicity and they can be used to calculate the scattered amplitude or the corresponding density function of any direct or reciprocal object, respectively. For example, Eq. 2.128 results in the atomic scattering factor, y(sin0/X.) isolated atom. In this case, p(x) is the electron density distribution in the atom, which is usually obtained fi om quantum mechanics. [Pg.238]

In the following we briefly discuss both approaches in more detail. It has been shown that the calculation of the amplitude for lepton scattering in the field of ultrarelativistic colliding nuclei can be performed exactly (Eichmann 2000 Eichmann et al. 2000a). The interaction part of the Dirac Hamiltonian (1.7) for two colliding nuclei, referred to by the subscripts (1) and (2) , at infinite energy y — oo reads... [Pg.24]

We shall continue with an example of the method of uniform approximation which is the correct theoretical method for calculating the scattering amplitude, including the interference as well as the rainbow, the glory or the forward diffraction contribution. Only the orbiting has to be described by other methods due to the quite different nature of this phenomenon (see, for instance, Berry and Mount, 1972). [Pg.322]

FIG. 22 Dependence of scattering amplitudes of the fast (o) and slow ( ) mode on solution ionic strength. Both added salt (NaCl) and free counterions are included in the calculation of ionic strength. Amplitudes represent excess scattering and are expressed in units of the scattering intensity of a benzene standard. Sodium poly(styrene sulfonate) (NaPSS), Mw = 5,000, polyion concentration c = 5 g/L, scattering angle 6 = 90°. (Adapted from Ref. 12.)... [Pg.48]

Within the framework of perturbative quantum field theory, there is a sharp contrast between the beautiful methods available for the calculation of collision amplitudes and those used in practice for the calculation of the properties of composite systems or "bound states," especially in the case of a gauge theory such as QED. As an example, consider the scattering of two particles, "1" and "2",... [Pg.435]

L. E DiMauro and P. Agostini Infrared Spectroscopy of Size Selected Molecular Clusters, U. Buck Femtosecond Spectroscopy of Molecules and Clusters, T. Baumer and G. Gerber Calculation of Electron Scattering on Hydrogenic Targets, /. Bray and A. T. Stelbovics Relativistic Calculations of Transition Amplitudes in the Helium Isoelectronic Sequence, W R. Johnson, D.R. Plante, and J. Sapirstein... [Pg.423]

For particles comprised of two or more types of materials, the scattered intensity needs to be calculated taking into account the interference between the different parts. For that it is more convenient to work in terms of scattering amplitudes defined in... [Pg.90]

The calculation of the diffracted intensities usually proceeds in two steps. The first step is the construction of the crystal potential and the calculation of the scattering amplitudes from a single atom, and the second step is the calculation of scattering processes within a single atomic layer and the calculation of scattering between different atomic layers. In the second step the multiple scattering processes are based on the condition that the scattered wave from one atom is an incident wave on all other atoms. This leads to a set of linear equations that is solved by matrix inversion. The formulation of the theory is based on the KKR (Korringa-Kohn-Rostocker) method used for band structure calculations. [Pg.4698]

Errors in Scattering Amplitudes and Errors Caused by Approximations in the Applied Theory. The calculation of complex scattering amplitudes (/) is discussed on p. 9 and p. 21. At least for light atoms (with atomic numbers less than say 20) published scattering amplitudes are quite accurate. For heavier atoms the atomic potentials are less well known, giving some inaccuracy in the/values. Table 4 shows the results obtained for the parameters in RuOj with two sets of scattering amplitudes for Ru. The... [Pg.42]

Eq. (IX.69) is the central RPA result for dense chain systems. It allows for detailed calculations of scattering by partly labeled chains. If the scattering amplitude of the nth monomer is a, the intensity scattered at a wave vector q has the form... [Pg.263]

Let us first recall how bound state problems like positronium m-e treated in the simpler theory of QED. First, we use perturbation theory to calculate a scattering amplitude between electron and positron. Then we identify a potential which will give the amplitude in Born approximation. Last, we substitute the potential in the wave equation, for example, the... [Pg.241]

The object of scattering theory is to calculate the scattering amplitude and cross section, given the interaction potentials between the two atoms. The first step in reducing the problem to practical computation is to introduce the partial wave expansion of the plane wave ... [Pg.489]

The calculation of scattering patterns is based on the summation of amplitudes or intensities scattered from all components. The intensity I of a wave described in the usual notation of complex variables is given by... [Pg.326]


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Scattering amplitude

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