The document presents information on collision phenomena and excitation and ionization processes in plasmas. It discusses various types of collisions including elastic and inelastic collisions. It also describes different ionization processes such as excitation and ionization by electron collisions, thermal ionization, Penning ionization, and photoionization. Processes of ion-ion and ion-electron recombination like radiative and dielectronic recombination are also summarized. The presentation contains diagrams and equations to illustrate key concepts and is intended to provide an overview of these plasma phenomena.
2. Contents
1. Collision phenomena
- Collision phenomena
- Velocity distribution
- Elastic and Inelastic collision
- Reaction cross-section
2. Ionization and Excitation
- Excitation and ionization by electron collision
- Excitation and ionization by energetic particles or neutral particles
- Thermal ionization
- Penning ionization
- Photo ionization and Photo excitation
- Ion – Ion recombination
- Ion-electron recombination
The most signicant difference between the Maxwellian energy distribution and the Druyvesteyn distribution is the different power of in the exponential argument. Physically, the Druyvesteyn distribution is specific to electrons interacting with neutrals of comparatively low energy. Figure is a graphical comparison between the Maxwellian and Druyvesteyn distributions.
The nuclear cross section of a nucleus is used to characterize the probability that a nuclear reaction will occur. The concept of a nuclear cross section can be quantified physically in terms of "characteristic area" where a larger area means a larger probability of interaction.
Recombination coefficient: 10^(-14) cm^3/s , 10^(-8) to 10^(-7), Te^(1/2), 10^(-7) to 10^(-6)