Electron Spin — Question 10

Section 40-2 · Physics pages 6610–6611

Question 10 Random phase noise reduces transverse polarization without changing z counts Initially |χ⟩= (| + z⟩+ | −z⟩)/ √ 2. In each trial the negative-z amplitude acquires a random phase ϕ drawn from a zero-mean Gaussian of variance v. Use ⟨eiϕ⟩= e−v/2. v |rx| Schematic; labels, not drawing lengths, specify the data. (a) Find the ensemble density matrix after phase averaging. (b) Find the positive-x probability and purity for v = 2 ln 2.
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Question 10 - Solution Random phase noise reduces transverse polarization without changing z counts v |rx| (a) Method and calculation ρ(ϕ) = 1 2 ( 1 e−iϕ eiϕ 1 ) . ¯ρ = 1 2 ( 1 e−v/2 e−v/2 1 ) . (b) Interpretation and further calculation v = 2 ln 2 : e−v/2 = 1/2 ⇒P+x = (1 + 1/2)/2 = 3/4 . Tr(¯ρ2) = (1 + e−v)/2 = 5/8 . Physical check Phase averaging preserves both z populations while suppressing off-diagonal terms. Purity falls because the unrecorded phases differ from trial to trial.

Question 10

Random phase noise reduces transverse polarization without changing z counts

Initially |χ⟩=(|+z⟩+|−z⟩)/2|\chi\rangle=(|+z\rangle+|-z\rangle)/\sqrt2. In each trial the negative-z amplitude acquires a random phase ϕ\phi drawn from a zero-mean Gaussian of variance vv. Use ⟨eiϕ⟩=e−v/2\langle e^{i\phi}\rangle=e^{-v/2}.

Diagram shown in the original SVG worksheet.

  1. Find the ensemble density matrix after phase averaging.

  2. Find the positive-x probability and purity for v=2ln⁡2v=2\ln2.

Question 10 - Solution

Random phase noise reduces transverse polarization without changing z counts

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ρ(ϕ)=12(1e−iϕeiϕ1).\rho(\phi)=\tfrac12\begin{pmatrix}1&e^{-i\phi}\\e^{i\phi}&1\end{pmatrix}.ρ‾=12(1e−v/2e−v/21).\boxed{\bar\rho=\tfrac12\begin{pmatrix}1&e^{-v/2}\\e^{-v/2}&1\end{pmatrix}}.

(b) Interpretation and further calculation

v=2ln⁡2:e−v/2=1/2⇒P+x=(1+1/2)/2=3/4.v=2\ln2:\quad e^{-v/2}=1/2\Rightarrow\boxed{P_{+x}=(1+1/2)/2=3/4}.Tr(ρ‾2)=(1+e−v)/2=5/8.\boxed{\mathrm{Tr}(\bar\rho^2)=(1+e^{-v})/2=5/8}.

Physical check

Phase averaging preserves both z populations while suppressing off-diagonal terms. Purity falls because the unrecorded phases differ from trial to trial.