Light as a Probability Wave — Question 1

Section 38-4 · Physics pages 6312–6313

Question 1 A lossless mixer converts a relative phase into complementary probabilities A single photon enters a two-path mixer with normalized amplitudes a = 1/ √ 2 and b = eiϕ/ √ 2. Output amplitudes are c+ = (a + b)/ √ 2 and c−= (a −b)/ √ 2. Detectors are ideal. a b + − Schematic; labels, not drawing lengths, specify the data. (a) Derive both output probabilities and check normalization. (b) Find the probabilities at ϕ = π/3 and explain what one detection records.
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Question 1 - Solution A lossless mixer converts a relative phase into complementary probabilities a b + − (a) Method and calculation c± = 1 2(1 ± eiϕ), P± = |c±|2. P± = 1 2(1 ± cos ϕ) , P+ + P−= 1. (b) Interpretation and further calculation ϕ = π/3 : P+ = 3/4, P−= 1/4 . (n+, n−) ∈{(1, 0), (0, 1)} for one photon . Physical check Probability amplitudes combine before taking the absolute square. A fractional probability is an ensemble prediction, not a fraction of a photon deposited at each ideal detector.

Question 1

A lossless mixer converts a relative phase into complementary probabilities

A single photon enters a two-path mixer with normalized amplitudes a=1/2a=1/\sqrt2 and b=eiϕ/2b=e^{i\phi}/\sqrt2. Output amplitudes are c+=(a+b)/2c_+=(a+b)/\sqrt2 and c−=(a−b)/2c_-=(a-b)/\sqrt2. Detectors are ideal.

Diagram shown in the original SVG worksheet.

  1. Derive both output probabilities and check normalization.

  2. Find the probabilities at ϕ=π/3\phi=\pi/3 and explain what one detection records.

Question 1 - Solution

A lossless mixer converts a relative phase into complementary probabilities

Diagram shown in the original SVG worksheet.

(a) Method and calculation

c±=12(1±eiϕ),P±=|c±|2.c_\pm=\tfrac12(1\pm e^{i\phi}),\quad P_\pm=|c_\pm|^2.P±=12(1±cos⁡ϕ),P++P−=1.\boxed{P_\pm=\tfrac12(1\pm\cos\phi)},\quad P_++P_-=1.

(b) Interpretation and further calculation

ϕ=π/3:P+=3/4,P−=1/4.\phi=\pi/3:\quad\boxed{P_+=3/4,\qquad P_-=1/4}.(n+,n−)∈{(1,0),(0,1)}for one photon.\boxed{(n_+,n_-)\in\{(1,0),(0,1)\}\quad\text{for one photon}}.

Physical check

Probability amplitudes combine before taking the absolute square. A fractional probability is an ensemble prediction, not a fraction of a photon deposited at each ideal detector.