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This article is about the concept in quantum mechanics. For the concept in classical mechanics, see Rotation

Spin is an intrinsic ⭕️ form of angular momentum carried by elementary particles, and thus by composite particles such as hadrons, atomic nuclei, and atoms.[1][2]: ⭕️ 183–184 Spin should not be conceptualized as involving the "rotation" of a particle's "internal mass", as ordinary use of the ⭕️ word may suggest: spin is a quantized property of waves.[3]

The existence of electron spin angular momentum is inferred from experiments, ⭕️ such as the Stern–Gerlach experiment, in which silver atoms were observed to possess two possible discrete angular momenta despite having ⭕️ no orbital angular momentum.[4] The existence of the electron spin can also be inferred theoretically from the spin–statistics theorem and ⭕️ from the Pauli exclusion principle—and vice versa, given the particular spin of the electron, one may derive the Pauli exclusion ⭕️ principle.

Spin is described mathematically as a vector for some particles such as photons, and as spinors and bispinors for other ⭕️ particles such as electrons. Spinors and bispinors behave similarly to vectors: they have definite magnitudes and change under rotations; however, ⭕️ they use an unconventional "direction". All elementary particles of a given kind have the same magnitude of spin angular momentum, ⭕️ though its direction may change. These are indicated by assigning the particle a spin quantum number.[2]: 183–184

The SI unit of ⭕️ spin is the same as classical angular momentum (i.e., N·m·s, J·s, or kg·m2·s−1). In practice, spin is usually given as ⭕️ a dimensionless spin quantum number by dividing the spin angular momentum by the reduced Planck constant ħ, which has the ⭕️ same dimensions as angular momentum. Often, the "spin quantum number" is simply called "spin".

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