The flat synchrotron spectra of partially self-absorbed jets revisited

Details The flat synchrotron spectra of partially self-absorbed jets revisited The flat synchrotron spectra of partially self-absorbed jets revisited

2006-01-05

arxiv.org/abs/astro-ph/0601103v1

Mon.Not.Roy.Astron.Soc. 367 (2006) 1083-1094

Astronomy and Astrophysics

Astrophysics

12 pages, 6 figures, accepted by MNRAS

Scientific paper

10.1111/j.1365-2966.2006.10030.x

Flat radio spectra with large brightness temperatures at the core of AGN and X-ray binaries are usually interpreted as the partially self-absorbed bases of jet flows emitting synchrotron radiation. Here we extend previous models of jets propagating at large angles to our line of sight to self-consistently include the effects of energy losses of the relativistic electrons due to the synchrotron process itself and the adiabatic expansion of the jet flow. We also take into account energy gains through self-absorption. Two model classes are presented. The ballistic jet flows, with the jet material travelling along straight trajectories, and adiabatic jets. Despite the energy losses, both scenarios can result in flat emission spectra, however, the adiabatic jets require a specific geometry. No re-acceleration process along the jet is needed for the electrons. We apply the models to observational data of the X-ray binary Cygnus X-1. Both models can be made consistent with the observations. The resulting ballistic jet is extremely narrow with a jet opening angle of only 5". Its energy transport rate is small compared to the time-averaged jet power and therefore suggests the presence of non-radiating protons in the jet flow. The adiabatic jets require a strong departure from energy equipartition between the magnetic field and the relativistic electrons. These models also imply a jet power two orders of magnitude higher than the Eddington limiting luminosity of a 10 solar mass black hole. The models put strong constraints on the physical conditions in the jet flows on scales well below achievable resolution limits.

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