Book contents
- Frontmatter
- Contents
- Preface
- 1 Introduction
- 2 Experimental techniques for cross-section measurements
- 3 Background quantum mechanics in the atomic context
- 4 One-electron problems
- 5 Theory of atomic bound states
- 6 Formal scattering theory
- 7 Calculation of scattering amplitudes
- 8 Spin-independent scattering observables
- 9 Spin-dependent scattering observables
- 10 Ionisation
- 11 Electron momentum spectroscopy
- References
- Index
7 - Calculation of scattering amplitudes
Published online by Cambridge University Press: 15 December 2009
- Frontmatter
- Contents
- Preface
- 1 Introduction
- 2 Experimental techniques for cross-section measurements
- 3 Background quantum mechanics in the atomic context
- 4 One-electron problems
- 5 Theory of atomic bound states
- 6 Formal scattering theory
- 7 Calculation of scattering amplitudes
- 8 Spin-independent scattering observables
- 9 Spin-dependent scattering observables
- 10 Ionisation
- 11 Electron momentum spectroscopy
- References
- Index
Summary
The background for the details of multichannel scattering calculations has now been established. We consider methods based on the integral-equation formulation of chapter 6. These momentum-space methods have proved accurate at all energies in a sufficient variety of situations to justify the belief that they can be generally applied. In some situations sufficient accuracy is achieved without resorting to the full power of the integral-equation solution. The methods used in these situations are distorted-wave methods. Their relationship to the full solutions will be examined in a simplified illustrative case. A brief outline will be given of alternative methods based on a coordinate-space formulation of the multichannel problem.
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.
We first show how to set up the problem within the framework of formal scattering theory using antisymmetric products of one-electron states. The problem is then formulated in terms of the calculation of reduced T-matrix elements relating the absolute values of initial and final momenta in different angular-momentum states. This depends on a knowledge of the corresponding potential matrix elements, whose calculation we treat in detail. We then show how the target continuum is accounted for in the scattering formalism.
- Type
- Chapter
- Information
- Electron-Atom Collisions , pp. 156 - 198Publisher: Cambridge University PressPrint publication year: 1995