Population can move between the levels by electron-impact excitation and de-excitation, spontaneous emission, radiative absorption and stimulated emission. Other collision partners and radiative cascades can matter in a fuller atom. In the elementary coronal approximation, the plasma is dilute, optically thin, steady, and weakly illuminated at the transition frequency. Electron impacts predominantly excite the lower level, while spontaneous emission predominantly empties the upper level; collisional de-excitation and photon trapping are negligible. The population balance isA key condition is neC21≪A21, together with insignificant external pumping and competing channels. A Maxwellian electron Maxwell-Boltzmann distribution lets the tabulated rate coefficient be expressed using one temperature.
neC12N1=A21N2,N1N2=A21neC12.
Ancestors (12)
- a
- 2
- S16
- 2019
- Past exam of the short options paper shared by Parts A and B of the physics course of the University of Oxford
- Short options paper shared by Parts A and B of the physics course of the University of Oxford
- Physics course of the University of Oxford
- Undergraduate course of the University of Oxford
- Course of the University of Oxford
- University of Oxford
- List of universities
- Home
Discussion (0)
New discussionThere are no discussions about this article yet.
Articles by others on the same topic (0)
There are currently no matching articles.