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

The existence of electron spin angular momentum is inferred from experiments, 1️⃣ such as the Stern–Gerlach experiment, in which silver atoms were observed to possess two possible discrete angular momenta despite having 1️⃣ no orbital angular momentum.[4] The existence of the electron spin can also be inferred theoretically from the spin–statistics theorem and 1️⃣ from the Pauli exclusion principle—and vice versa, given the particular spin of the electron, one may derive the Pauli exclusion 1️⃣ principle.

Spin is described mathematically as a vector for some particles such as photons, and as spinors and bispinors for other 1️⃣ particles such as electrons. Spinors and bispinors behave similarly to vectors: they have definite magnitudes and change under rotations; however, 1️⃣ they use an unconventional "direction". All elementary particles of a given kind have the same magnitude of spin angular momentum, 1️⃣ though its direction may change. These are indicated by assigning the particle a spin quantum number.[2]: 183–184

The SI unit of 1️⃣ 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 1️⃣ a dimensionless spin quantum number by dividing the spin angular momentum by the reduced Planck constant ħ, which has the 1️⃣ same dimensions as angular momentum. Often, the "spin quantum number" is simply called "spin".

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