The component along an arbitrary direction \(\widehat{n}\), with direction cosines (nx, ny, n2), of the spin of a spin -\(\frac{1}{2}\) particle is measured. The result is

1
0
2
±\(\frac{h}{2}\)n2
3
±\(\frac{h}{2}\)(nx + ny + n2)
4
±\(\frac{h}{2}\)

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