A silver atom is prepared in the state

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · The formalism of quantum mechanics · The formalism of quantum mechanics

The Structure of Quantum Mechanics, Ch The postulates, measurement and collapse

Problem

A silver atom is prepared in the state ∣↑⟩|{\uparrow}\rangle, the +ℏ/2+\hbar/2 eigenstate of S^z\hat S_z. It passes three stages in succession. Stage 1 measures S^x\hat S_x non-selectively: a detector on each output beam records which way each atom went, and neither beam is blocked. Stage 2 measures S^z\hat S_z selectively; only the +ℏ/2+\hbar/2 ("up") beam is kept. Stage 3 measures S^n\hat S_n selectively, where n^\hat n lies in the xzxz-plane at 60∘60^\circ to zz with +ℏ/2+\hbar/2 eigenstate ∣↑n⟩=cos⁡30∘ ∣↑⟩+sin⁡30∘ ∣↓⟩|{\uparrow}_n\rangle=\cos30^\circ\,|{\uparrow}\rangle+\sin30^\circ\,|{\downarrow}\rangle; only the +ℏ/2+\hbar/2 beam is kept. ((a)) Using the non-selective measurement rule (weight the probability of each later outcome by the Born probability of each recorded stage-1 outcome, applying the projection postulate for that outcome along the way), find the probability that stage 2 gives "up". ((b)) Given that stage 2 gives "up", state the normalised post-measurement state entering stage 3, and find the probability that stage 3 gives its +ℏ/2+\hbar/2 outcome. ((c)) Find the overall probability of the recorded sequence "up at stage 2, +ℏ/2+\hbar/2 at stage 3". Then explain, referring to the projection postulate, why the probability found in part (a) differs from the probability of getting "up" at stage 2 if stage 1 were omitted entirely.

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