The Stern-Gerlach Experiment — Question 7

Section 40-4 · Physics pages 6644–6645

Question 7 Discarding the analyzer record differs from undoing its interaction Initially the spin is | + x⟩= (| + z⟩+ | −z⟩)/ √ 2. A z analyzer correlates the states with orthogonal paths A and B. In case I the path information is irreversibly discarded; in case II the analyzer interaction is exactly reversed before detection. +z, A −z, B Schematic; labels, not drawing lengths, specify the data. (a) Find the reduced spin state in case I and the positive-x probability. (b) Find the positive-x probability in case II.
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Question 7 - Solution Discarding the analyzer record differs from undoing its interaction +z, A −z, B (a) Method and calculation |Ψ⟩= (| + z, A⟩+ | −z, B⟩)/ √ 2, ⟨A|B⟩= 0. ρspin = Trpath|Ψ⟩⟨Ψ| = I/2 ⇒PI(+x) = 1/2 . (b) Interpretation and further calculation U−1|Ψ⟩= | + x⟩|input path⟩. PII(+x) = 1 . Physical check Exact reversal includes phase control and erasure of every path record. Merely bringing two incoherent beams to the same location does not restore their spin coherence.

Question 7

Discarding the analyzer record differs from undoing its interaction

Initially the spin is |+x⟩=(|+z⟩+|−z⟩)/2|+x\rangle=(|+z\rangle+|-z\rangle)/\sqrt2. A z analyzer correlates the states with orthogonal paths A and B. In case I the path information is irreversibly discarded; in case II the analyzer interaction is exactly reversed before detection.

Diagram shown in the original SVG worksheet.

  1. Find the reduced spin state in case I and the positive-x probability.

  2. Find the positive-x probability in case II.

Question 7 - Solution

Discarding the analyzer record differs from undoing its interaction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

|Ψ⟩=(|+z,A⟩+|−z,B⟩)/2,⟨A|B⟩=0.|\Psi\rangle=(|+z,A\rangle+|-z,B\rangle)/\sqrt2,\quad\langle A|B\rangle=0.ρspin=Trpath|Ψ⟩⟨Ψ|=I/2⇒PI(+x)=1/2.\rho_{\mathrm{spin}}=\mathrm{Tr}_{\mathrm{path}}|\Psi\rangle\langle\Psi|=I/2\Rightarrow\boxed{P_I(+x)=1/2}.

(b) Interpretation and further calculation

U−1|Ψ⟩=|+x⟩|input path⟩.U^{-1}|\Psi\rangle=|+x\rangle|\text{input path}\rangle.PII(+x)=1.\boxed{P_{II}(+x)=1}.

Physical check

Exact reversal includes phase control and erasure of every path record. Merely bringing two incoherent beams to the same location does not restore their spin coherence.