Intensity in Double-Slit Interference — Question 6

Section 35-5 · Physics pages 5802–5803

Question 6 A finite detector pixel averages over part of a fringe The local pattern is I(y) = A[1 + V0 cos(2πy/p)], where p is the fringe spacing. A uniform rectangular pixel of width w centered at y0 reports the spatial average across its width. y I w Schematic; labels, not drawing lengths, specify the data. (a) Integrate the signal and derive the recorded visibility. (b) For V0 = 1 and w = p/2, find the recorded visibility; determine the first positive w that removes all modulation.
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Question 6 - Solution A finite detector pixel averages over part of a fringe y I w (a) Method and calculation I(y0) = 1 w Z y0+w/2 y0−w/2 I(y)dy. I = A  1 + V0 sin(πw/p) πw/p cos(2πy0/p)  . (b) Interpretation and further calculation Vpixel = V0 sin(πw/p) πw/p ; w = p/2 ⇒Vpixel = 2/π . πw/p = π =⇒w = p at the first zero . Physical check A detector can report poor contrast even for a perfectly coherent optical field if its pixels integrate over a significant fraction of a fringe.

Question 6

A finite detector pixel averages over part of a fringe

The local pattern is I(y)=A[1+V0cos⁡(2πy/p)]I(y)=A[1+V_0\cos(2\pi y/p)], where p is the fringe spacing. A uniform rectangular pixel of width w centered at y0y_0 reports the spatial average across its width.

Diagram shown in the original SVG worksheet.

  1. Integrate the signal and derive the recorded visibility.

  2. For V0=1V_0=1 and w=p/2w=p/2, find the recorded visibility; determine the first positive w that removes all modulation.

Question 6 - Solution

A finite detector pixel averages over part of a fringe

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I¯(y0)=1w∫y0−w/2y0+w/2I(y)dy.\overline I(y_0)=\frac1w\int_{y_0-w/2}^{y_0+w/2}I(y)dy.I¯=A[1+V0sin⁡(πw/p)πw/pcos(2πy0/p)].\boxed{\overline I=A\left[1+V_0\frac{\sin(\pi w/p)}{\pi w/p}\cos(2\pi y_0/p)\right]}.

(b) Interpretation and further calculation

Vpixel=V0|sin⁡(πw/p)πw/p|;w=p/2⇒Vpixel=2/π.\boxed{V_{\mathrm{pixel}}=V_0\left|\frac{\sin(\pi w/p)}{\pi w/p}\right|};\quad w=p/2\Rightarrow\boxed{V_{\mathrm{pixel}}=2/\pi}.πw/p=π⇒w=pat the first zero.\pi w/p=\pi\Longrightarrow\boxed{w=p\ \text{at the first zero}}.

Physical check

A detector can report poor contrast even for a perfectly coherent optical field if its pixels integrate over a significant fraction of a fringe.