quantum angular momentum
Angular momentum is the physics of spinning and orbiting — the quantity that keeps a top upright and a planet circling the Sun. In everyday life it can take any value you like; a wheel can turn slowly or fast by any amount. In the quantum world the story changes: a particle's rotational motion comes only in discrete, countable amounts set by the constant ℏ (h-bar, Planck's constant divided by 2π). You cannot dial it smoothly; you must climb a ladder of allowed values.
This quantization is not a quirk of any one experiment but a deep feature of how rotation works for waves. Because a quantum particle is described by a wavefunction that must join up smoothly when you go all the way around a circle, only certain whole-number patterns fit. Those patterns fix both how much angular momentum the particle has and how it can point. The result is the orderly structure behind atomic orbitals, molecular rotation, and the colours atoms emit.
It is worth being honest about the picture in your head. A quantum particle with angular momentum is not literally a tiny ball whirling on a string; the wavefunction is a probability amplitude spread through space, and angular momentum measures a rotational property of that amplitude. The numbers it can take are real and measurable, but the cosy mental image of a spinning marble is a helpful crutch, not the underlying reality.
The magnitude of orbital angular momentum is fixed by a whole number ℓ and the quantum of action ℏ.
There are two distinct kinds of quantum angular momentum: orbital, from a particle's motion through space, and spin, an intrinsic property with no spinning-ball counterpart. This entry is the umbrella idea; spin gets its own treatment.