Book contents
- Frontmatter
- Contents
- Preface
- 1 Introduction
- 2 Single electron transition probabilities
- 3 Formulation of multi-electron transition probabilities
- 4 Independent electron approximation
- 5 Statistical methods
- 6 Correlated multi-electron electron transition probabilities
- 7 Perturbation expansions
- 8 Projectiles carrying electrons
- 9 Reactions with photons
- 10 Relations between charged particle and photon reactions
- Appendices
- References
- Index
9 - Reactions with photons
Published online by Cambridge University Press: 11 September 2009
- Frontmatter
- Contents
- Preface
- 1 Introduction
- 2 Single electron transition probabilities
- 3 Formulation of multi-electron transition probabilities
- 4 Independent electron approximation
- 5 Statistical methods
- 6 Correlated multi-electron electron transition probabilities
- 7 Perturbation expansions
- 8 Projectiles carrying electrons
- 9 Reactions with photons
- 10 Relations between charged particle and photon reactions
- Appendices
- References
- Index
Summary
Introduction
In this chapter interactions of photons with atoms are considered. Here the emphasis is on systems interacting with weak electromagnetic fields so that a single atomic electron interacts with a single photon. Initially interactions with a single electron are considered. In this case the photon tends to probe in a comparatively delicate way the details of the atomic wavefunction (e.g. effects of static correlation in multi-electron atoms). Later two electron transitions are considered. Because these two electron transitions are often negligible in the absence of electron correlation the two electron transitions are usually a direct probe of the dynamics of electron correlation.
In previous chapters the impact parameter (or particle) picture has been used wherever possible in order to recover the product form for the transition probability in the limit of zero correlation. However, here the likelihood of interacting with more than a single photon is quite small since the electromagnetic field of a photon, even for strong laser fields, is almost always small compared with the electric field provided by the target nucleus. Consequently, this independent electron limit is not often useful. Also, photon wavepackets are usually much larger in size than an atom. Consequently the wave picture is used where the electric and magnetic fields of the photon are considered to be plane waves. Transformation to the particle picture may be done using the usual Fourier transform from the scattering amplitude to the probability amplitude (Cf. section 3.3.3).
- Type
- Chapter
- Information
- Electron Correlation Dynamics in Atomic Collisions , pp. 198 - 228Publisher: Cambridge University PressPrint publication year: 1997