Light as a Probability Wave — Question 2

Section 38-4 · Physics pages 6314–6315

Question 2 Fringe visibility reveals path imbalance with a labeling ambiguity At a lossless mixer, the input amplitudes are a = √p and b = √1 −p eiϕ, with 0 ≤p ≤1. One output has amplitude (a + b)/ √ 2. Visibility is V = (Pmax −Pmin)/(Pmax + Pmin). a b + − Schematic; labels, not drawing lengths, specify the data. (a) Derive the phase-dependent detection probability and visibility. (b) Infer all possible values of p from V = .800.
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Question 2 - Solution Fringe visibility reveals path imbalance with a labeling ambiguity a b + − (a) Method and calculation P(ϕ) = 1 2 [1 + 2 √ p(1 −p) cos ϕ ]. Pmax,min = 1 2 ± √ p(1 −p), V = 2 √ p(1 −p) . (b) Interpretation and further calculation p(1 −p) = .160 ⇒ p2 −p + .160 = 0. p = .200 or .800 . Physical check Visibility cannot identify which input path carries the larger probability. An additional path-resolved measurement is required to break that symmetry.

Question 2

Fringe visibility reveals path imbalance with a labeling ambiguity

At a lossless mixer, the input amplitudes are a=pa=\sqrt p and b=1−peiϕb=\sqrt{1-p}\,e^{i\phi}, with 0≤p≤10\le p\le1. One output has amplitude (a+b)/2(a+b)/\sqrt2. Visibility is 𝒱=(Pmax−Pmin)/(Pmax+Pmin)\mathcal V=(P_{\max}-P_{\min})/(P_{\max}+P_{\min}).

Diagram shown in the original SVG worksheet.

  1. Derive the phase-dependent detection probability and visibility.

  2. Infer all possible values of p from 𝒱=.800\mathcal V=.800.

Question 2 - Solution

Fringe visibility reveals path imbalance with a labeling ambiguity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

P(ϕ)=12[1+2p(1−p)cos⁡ϕ].P(\phi)=\tfrac12\bigl[1+2\sqrt{p(1-p)}\cos\phi\bigr].Pmax⁡,min=12±p(1−p),𝒱=2p(1−p).P_{\max,\min}=\tfrac12\pm\sqrt{p(1-p)},\quad\boxed{\mathcal V=2\sqrt{p(1-p)}}.

(b) Interpretation and further calculation

p(1−p)=.160⇒p2−p+.160=0.p(1-p)=.160\quad\Rightarrow\quad p^2-p+.160=0.p=.200or.800.\boxed{p=.200\ \text{or}\ .800}.

Physical check

Visibility cannot identify which input path carries the larger probability. An additional path-resolved measurement is required to break that symmetry.