Synchrotron radiation is a key process in the radio emission from active galactic nuclei (AGNs). It is produced when fast-moving electrons spiral around magnetic field lines, emitting energy as they accelerate. This process is especially important in the radio bands but becomes less significant at higher energies like X-rays and gamma rays. Why does this happen?
A charged particle (like an electron) moving in a magnetic field B experiences a force that makes it spiral, emitting radiation. For very fast (relativistic) electrons, this is called synchrotron radiation.
The force is given by:
F = q (v × B)
The typical frequency of synchrotron radiation is:
νsync ≈ γ² (e B) / (2π me c)
Higher energy electrons and stronger magnetic fields produce higher frequency radiation.
Electrons lose energy as they emit synchrotron radiation. The cooling timescale is:
tsync ≈ 6π me c / (σT γ B²)
Electrons that could emit X-rays or gamma rays lose energy too fast to fill large regions.
Take an electron with γ = 1000 in a magnetic field of B = 100 μG. Plug into:
νsync ≈ γ² (e B) / (2π me c)
Calculate:
νsync ≈ 106 × (2.8 × 106 Hz) ≈ 2.8 GHz
This aligns perfectly with observed AGN jet radio emission.
Regime | Synchrotron? | Examples |
---|---|---|
Radio | Yes | AGN jets, supernovae |
Infrared | Yes | Starbursts, AGN tori |
Optical | Sometimes | M87 jet, blazars |
X-ray | Rare | Crab Nebula, GRB afterglows |
Gamma-ray | No | Usually other processes |
Synchrotron radiation dominates the radio emission from AGNs because electrons can emit at these frequencies for long times and over large regions. At higher energies, electrons lose energy too quickly, so other processes become more important.