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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馃挾 form of angular momentum carried by elementary particles, and thus by composite particles such as hadrons, atomic nuclei, and atoms.[1][2]:馃挾 183鈥?84 Spin should not be conceptualized as involving the "rotation" of a particle's "internal mass", as ordinary use of the馃挾 word may suggest: spin is a quantized property of waves.[3]
The existence of electron spin angular momentum is inferred from experiments,馃挾 such as the Stern鈥揋erlach experiment, in which silver atoms were observed to possess two possible discrete angular momenta despite having馃挾 no orbital angular momentum.[4] The existence of the electron spin can also be inferred theoretically from the spin鈥搒tatistics theorem and馃挾 from the Pauli exclusion principle鈥攁nd vice versa, given the particular spin of the electron, one may derive the Pauli exclusion馃挾 principle.
Spin is described mathematically as a vector for some particles such as photons, and as spinors and bispinors for other馃挾 particles such as electrons. Spinors and bispinors behave similarly to vectors: they have definite magnitudes and change under rotations; however,馃挾 they use an unconventional "direction". All elementary particles of a given kind have the same magnitude of spin angular momentum,馃挾 though its direction may change. These are indicated by assigning the particle a spin quantum number.[2]: 183鈥?84
The SI unit of馃挾 spin is the same as classical angular momentum (i.e., N路m路s, J路s, or kg路m2路s鈭?). In practice, spin is usually given as馃挾 a dimensionless spin quantum number by dividing the spin angular momentum by the reduced Planck constant 魔, which has the馃挾 same dimensions as angular momentum. Often, the "spin quantum number" is simply called "spin".
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