The spin projection is the component of a particle's spin angular momentum along a specified spatial direction. For the direction, an eigenstate of the angular momentum operator has measured value , where and is the reduced Planck constant. For spin one-half, the two possible results are and .
The direction belongs to the measurement arrangement: a state with definite generally has uncertain . A Stern-Gerlach experiment separates the corresponding components through a spatially varying magnetic field. This is a component measurement, rather than a claim that the full spin angular momentum points along one of two classical directions.
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