Electron Spin — Question 9

Section 40-2 · Physics pages 6608–6609

Question 9 A full spin rotation can change an interferometer output An ideal two-path interferometer recombines equal amplitudes with zero initial relative phase. Only path A applies Uz(θ) = exp(−iθσz/2) to an incident | + z⟩. The probability at its initially bright output is P = |(1 + u)/2|2, where Uz| + z⟩= u| + z⟩. A: Uz(θ) B: reference Schematic; labels, not drawing lengths, specify the data. (a) Find P as a function of the rotation angle. (b) Compare θ = 2π and 4π, and explain why the phase is observable here.
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Question 9 - Solution A full spin rotation can change an interferometer output A: Uz(θ) B: reference (a) Method and calculation σz| + z⟩= | + z⟩⇒u = e−iθ/2. P = 1 4(2 + 2 cos(θ/2)) = cos2(θ/4) . (b) Interpretation and further calculation P(2π) = 0, P(4π) = 1 . 2π : |A⟩+ |B⟩−→−|A⟩+ |B⟩. Physical check A phase applied to only one path is relative to the other path. Rotating both paths identically would produce only a common phase and no intensity change.

Question 9

A full spin rotation can change an interferometer output

An ideal two-path interferometer recombines equal amplitudes with zero initial relative phase. Only path A applies Uz(θ)=exp⁡(−iθσz/2)U_z(\theta)=\exp(-i\theta\sigma_z/2) to an incident |+z⟩|+z\rangle. The probability at its initially bright output is P=|(1+u)/2|2P=|(1+u)/2|^2, where Uz|+z⟩=u|+z⟩U_z|+z\rangle=u|+z\rangle.

Diagram shown in the original SVG worksheet.

  1. Find P as a function of the rotation angle.

  2. Compare θ=2π\theta=2\pi and 4π4\pi, and explain why the phase is observable here.

Question 9 - Solution

A full spin rotation can change an interferometer output

Diagram shown in the original SVG worksheet.

(a) Method and calculation

σz|+z⟩=|+z⟩⇒u=e−iθ/2.\sigma_z|+z\rangle=|+z\rangle\Rightarrow u=e^{-i\theta/2}.P=14(2+2cos⁡(θ/2))=cos⁡2(θ/4).P=\tfrac14(2+2\cos(\theta/2))=\boxed{\cos^2(\theta/4)}.

(b) Interpretation and further calculation

P(2π)=0,P(4π)=1.\boxed{P(2\pi)=0,\quad P(4\pi)=1}.2π:|A⟩+|B⟩→−|A⟩+|B⟩.2\pi:\quad |A\rangle+|B\rangle\longrightarrow-|A\rangle+|B\rangle.

Physical check

A phase applied to only one path is relative to the other path. Rotating both paths identically would produce only a common phase and no intensity change.