| dc.contributor.author | Krishan, V | |
| dc.contributor.author | Wiita, P. J | |
| dc.date.accessioned | 2008-09-15T14:47:46Z | |
| dc.date.available | 2008-09-15T14:47:46Z | |
| dc.date.issued | 1990-10 | |
| dc.identifier.citation | Monthly Notices of Royal Astronomical Society, Vol. 246, No. 4, pp. 597 - 607 | en |
| dc.identifier.issn | 0035-8711 | |
| dc.identifier.uri | http://hdl.handle.net/2248/3627 | |
| dc.description.abstract | Stimulated Raman scattering processes appear to be able to produce the typical electromagnetic continuum of an active galactic nucleus (AGN). Seed photons beat through Raman forward-scattering to create Langmuir plasma waves which can quickly accelerate electrons to Lorentz factors of 10^3^ to 10^4^. These electrons radiate their energy through Raman back- scattering off magnetic fields engendered by magnetic modulational instabilities afflicting the Langmuir waves. The frequency of emission is proportional to the square root of the ambient density, so γ-rays can be produced in the highest density regions near the central engine, with X-rays through to IR photons produced at greater distances. Both the high luminosity and broken power-law continuum characteristic of an AGN emerge from reasonable density distributions. Bremsstrahlung emission in the UV is a by-product of this mechanism and could explain the 'blue bump'. Because the electrons are continuously accelerated in this picture, a steady-state distribution arises naturally and a simple relation exists between the density of the relativistic particles which emit the radiation and the ambient plasma density which is involved in the acceleration. | en |
| dc.language.iso | en | en |
| dc.publisher | Royal Astronomical Society | en |
| dc.relation.uri | http://ads.iucaa.ernet.in/abs/1990MNRAS.246..597K | en |
| dc.subject | Plasma Processes | en |
| dc.subject | Emission in Galactic Nuclei | en |
| dc.title | Coherent Plasma Processes and the Continuum Emission in Active Galactic Nuclei | en |
| dc.type | Article | en |