High-mass stars: supernova & remnants
- After the red supergiant phase, successive fusion rounds (C, Ne, Mg, Si...) build an onion-layered star around an iron core — iron can't release net energy by fusing.
- Core collapses catastrophically; infalling gas rebounds off the dense core → Type II supernova (rapid rise in absolute magnitude, briefly rivalling the full moon).
- Remnant becomes either a neutron star or a black hole, depending on the leftover mass.
Neutron stars & pulsars
p + e → n + ν_e
- Neutron degeneracy pressure halts collapse; density ≈10¹⁷ kg m⁻³ (nuclear density) — a 1.4 M☉ neutron star is only ~10 km across.
- Rapid spin (angular momentum conservation) + intense magnetic field → beamed radio emission. If the beam sweeps past Earth, it's observed as a regular pulsar.
Black holes
The event horizon is a boundary, not a point.
Core mass >~10 M☉ → even neutron degeneracy pressure fails → collapse to a singularity. The event horizon is the boundary where escape velocity = c; its radius is the Schwarzschild radius, R_s≈2GM/c².
Supermassive black holes (millions of M☉) sit at galaxy centres (e.g. Sagittarius A*). Actively feeding ones form a hot accretion disc — seen as a quasar.