Light as a Probability Wave — Question 8

Section 38-4 · Physics pages 6326–6327

Question 8 Finite detector pixels average a probability fringe before counting Across a small region of a broad beam, the density is p(x) = p0[1 + cos(kx)], with constant envelope p0 and k > 0. A pixel of width d is centered at x0 and lies entirely in that region. The full beam is normalized elsewhere. x p(x) d Schematic; labels, not drawing lengths, specify the data. (a) Integrate p over the pixel and derive the visibility as its center is scanned. (b) Evaluate the visibility for d = π/k and d = 2π/k.
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Question 8 - Solution Finite detector pixels average a probability fringe before counting x p(x) d (a) Method and calculation Ppix = Z x0+d/2 x0−d/2 p(x)dx = p0d  1 + sin(kd/2) kd/2 cos(kx0)  . Vpix = sin(kd/2) kd/2 . (b) Interpretation and further calculation d = π/k : Vpix = 2/π = .636620 . d = 2π/k : Vpix = 0 . Physical check Loss of measured contrast here comes from spatial averaging, not from loss of coherence of the incident photon state.

Question 8

Finite detector pixels average a probability fringe before counting

Across a small region of a broad beam, the density is p(x)=p0[1+cos⁡(kx)]p(x)=p_0[1+\cos(kx)], with constant envelope p0p_0 and k>0k>0. A pixel of width d is centered at x0x_0 and lies entirely in that region. The full beam is normalized elsewhere.

Diagram shown in the original SVG worksheet.

  1. Integrate p over the pixel and derive the visibility as its center is scanned.

  2. Evaluate the visibility for d=π/kd=\pi/k and d=2π/kd=2\pi/k.

Question 8 - Solution

Finite detector pixels average a probability fringe before counting

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ppix=∫x0−d/2x0+d/2p(x)dx=p0d[1+sin⁡(kd/2)kd/2cos(kx0)].P_{\mathrm{pix}}=\int_{x_0-d/2}^{x_0+d/2}p(x)dx=p_0d\left[1+\frac{\sin(kd/2)}{kd/2}\cos(kx_0)\right].𝒱pix=|sin⁡(kd/2)kd/2|.\boxed{\mathcal V_{\mathrm{pix}}=\left|\frac{\sin(kd/2)}{kd/2}\right|}.

(b) Interpretation and further calculation

d=π/k:𝒱pix=2/π=.636620.d=\pi/k:\quad\boxed{\mathcal V_{\mathrm{pix}}=2/\pi=.636620}.d=2π/k:𝒱pix=0.d=2\pi/k:\quad\boxed{\mathcal V_{\mathrm{pix}}=0}.

Physical check

Loss of measured contrast here comes from spatial averaging, not from loss of coherence of the incident photon state.