Light as a Probability Wave — Question 6

Section 38-4 · Physics pages 6322–6323

Question 6 Discrete detection amplitudes require normalization before conditioning A photon is in three mutually exclusive orthonormal detection modes with amplitudes A(1, 2i, −1). Take A real and positive. Detectors distinguish all three modes perfectly. D1 D2 D3 Schematic; labels, not drawing lengths, specify the data. (a) Normalize the state and find the three detection probabilities. (b) Given that mode 2 did not click, find the conditional probability of mode 3.
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Question 6 - Solution Discrete detection amplitudes require normalization before conditioning D1 D2 D3 (a) Method and calculation 1 = |A|2(1 + 4 + 1) ⇒ A = 1/ √ 6 . (P1, P2, P3) = (1/6, 2/3, 1/6) . (b) Interpretation and further calculation P(not 2) = P1 + P3 = 1/3. P(3 | not 2) = P3 P1 + P3 = 1/2 . Physical check The minus sign and the factor i matter if the modes are later mixed coherently; they do not change probabilities of this direct mode-resolving measurement.

Question 6

Discrete detection amplitudes require normalization before conditioning

A photon is in three mutually exclusive orthonormal detection modes with amplitudes A(1,2i,−1)A(1,2i,-1). Take A real and positive. Detectors distinguish all three modes perfectly.

Diagram shown in the original SVG worksheet.

  1. Normalize the state and find the three detection probabilities.

  2. Given that mode 2 did not click, find the conditional probability of mode 3.

Question 6 - Solution

Discrete detection amplitudes require normalization before conditioning

Diagram shown in the original SVG worksheet.

(a) Method and calculation

1=|A|2(1+4+1)⇒A=1/6.1=|A|^2(1+4+1)\quad\Rightarrow\quad\boxed{A=1/\sqrt6}.(P1,P2,P3)=(1/6,2/3,1/6).\boxed{(P_1,P_2,P_3)=(1/6,2/3,1/6)}.

(b) Interpretation and further calculation

P(not 2)=P1+P3=1/3.P(\text{not }2)=P_1+P_3=1/3.P(3∣not 2)=P3P1+P3=1/2.\boxed{P(3\mid\text{not }2)=\frac{P_3}{P_1+P_3}=1/2}.

Physical check

The minus sign and the factor i matter if the modes are later mixed coherently; they do not change probabilities of this direct mode-resolving measurement.