relativistic beaming
Imagine a lawn sprinkler that sprays water evenly in all directions. Now mount it on a fast-moving truck. To someone standing by the road, the spray no longer goes everywhere equally — it gets swept forward into a tight cone pointing the way the truck is heading. Relativistic beaming is this same effect for the radiation and particles emitted by something moving close to the speed of light: what would spray out in all directions instead gets focused sharply forward.
The cause is the way relativity mixes up angles between frames. A source moving near light speed might, in its own rest frame, emit light or particles evenly in every direction. But when you transform to the lab frame, those directions are crowded together toward the forward direction, and the forward-going radiation is also blueshifted and brightened. The faster the source — the higher its Lorentz factor gamma — the narrower the forward cone, with a half-angle that shrinks roughly as one over gamma. This is sometimes called the headlight effect, because the emission is concentrated like a beam from a headlamp.
Relativistic beaming is everywhere once particles go fast. In synchrotrons and storage rings, electrons swung around in circles emit their light in a tight forward sweep, which is exactly why synchrotron light sources are so brilliant and useful. In astrophysics, jets of plasma blasting out of black holes at near-light speed appear enormously brighter when they happen to point toward Earth, an effect that explains why some galaxies and the relativistic jets called blazars look so extreme. The same physics, one cause: motion near c bunches emission forward.
Emission from a source with Lorentz factor gamma is squeezed into a forward cone of half-angle roughly 1/gamma. At gamma = 100, that cone is only about half a degree wide.
The faster the source, the tighter its emission is focused forward — the headlight effect.
Beaming concerns the directions of emission, while the relativistic Doppler effect concerns its frequency or energy; both come from the same Lorentz transformation and usually occur together for a fast-moving source.