Abstract

Under the assumption that we can create in the laboratory any electromagnetic field consistent with Maxwell’s equations, it is shown that an arbitrary Hermitian operator on a spin system can be measured using a suitable generalization of the Stern–Gerlach experiment. In particular, it is shown that every proposition about the spin-1 system is verifiable, answering the challenge of Hultgren and Shimony. The analysis also reveals complications in the standard Stern–Gerlach experiment of which many physicists are apparently not aware.

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