Suppose that at the channel's outgoing end in the hydrogen (ℓ = 0) Stern-Gerlach apparatus of Figure 8.3, you place a second such apparatus whose channel is aligned with the first but rotated 90° about the x-axis, so that its B-field lines point roughly in the y-direction instead of the z. What would you see emerging at the end of your added apparatus? Consider the behavior of the spin-up and spin-down beams separately. Assume that when these beams are separated in the first apparatus, we can choose to block one or the other for study, but also assume that neither is deviated too far from the center of the channel.
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