In quantum mechanics, the **angular momentum operator** is one of several related operators analogous to classical angular momentum. The angular momentum operator plays a central role in the theory of atomic physics and other quantum problems involving rotational symmetry. In both classical and quantum mechanical systems, angular momentum (together with linear momentum and energy) is one of the three fundamental properties of motion.

There are several angular momentum operators: **total angular momentum** (usually denoted **J**), **orbital angular momentum** (usually denoted **L**), and **spin angular momentum** (**spin** for short, usually denoted **S**). The term "angular momentum operator" can (confusingly) refer to either the total or the orbital angular momentum. Total angular momentum is always conserved, due to Noether's theorem.

Read more about Angular Momentum Operator: Spin, Orbital, and Total Angular Momentum, Orbital Angular Momentum Operator, Quantization, Angular Momentum As The Generator of Rotations, Conservation of Angular Momentum, Angular Momentum Coupling, Orbital Angular Momentum in Spherical Coordinates

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