Gratings: Dispersion and Resolving Power — Question 7

Section 36-8 · Physics pages 6004–6005

Question 7 Pixel sampling and optical resolution impose separate wavelength scales A first-order grating has d = 1.00 µm, N=5000, and central wavelength 600 nm. A centered camera has f = 0.200 m and pixel pitch p = 10.0 µm. Require at least two pixels across a resolved spectral interval. p spectral detector Schematic; labels, not drawing lengths, specify the data. (a) Find the wavelength interval corresponding to two pixels. (b) Compare it with the ideal diffraction resolution and identify the larger limiting scale.
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Question 7 - Solution Pixel sampling and optical resolution impose separate wavelength scales p spectral detector (a) Method and calculation sin θ = 0.600, cos θ = 0.800 =⇒D = 1.25 × 106 rad/m. ∆λ2p = 2p/(fD) = 0.0800 nm . (b) Interpretation and further calculation ∆λd = λ/N = 600/5000 = 0.120 nm . ∆λd > ∆λ2p =⇒diffraction is the larger limit; its width spans 3 pixels . Physical check Fine pixels can sample an optical line well, but they cannot recover spectral detail removed by the optical response.

Question 7

Pixel sampling and optical resolution impose separate wavelength scales

A first-order grating has d=1.00μmd=1.00\,\mu\mathrm m, N=5000, and central wavelength 600nm600\,\mathrm{nm}. A centered camera has f=0.200mf=0.200\,\mathrm m and pixel pitch p=10.0μmp=10.0\,\mu\mathrm m. Require at least two pixels across a resolved spectral interval.

Diagram shown in the original SVG worksheet.

  1. Find the wavelength interval corresponding to two pixels.

  2. Compare it with the ideal diffraction resolution and identify the larger limiting scale.

Question 7 - Solution

Pixel sampling and optical resolution impose separate wavelength scales

Diagram shown in the original SVG worksheet.

(a) Method and calculation

sin⁡θ=0.600,cos⁡θ=0.800⇒𝒟=1.25×106rad/m.\sin\theta=0.600,\quad\cos\theta=0.800\Longrightarrow\mathcal D=1.25\times10^6\,\mathrm{rad/m}.Δλ2p=2p/(f𝒟)=0.0800nm.\boxed{\Delta\lambda_{2p}=2p/(f\mathcal D)=0.0800\,\mathrm{nm}}.

(b) Interpretation and further calculation

Δλd=λ/N=600/5000=0.120nm.\boxed{\Delta\lambda_d=\lambda/N=600/5000=0.120\,\mathrm{nm}}.Δλd>Δλ2p⇒diffraction is the larger limit; its width spans 3 pixels.\Delta\lambda_d>\Delta\lambda_{2p}\Longrightarrow\boxed{\text{diffraction is the larger limit; its width spans }3\text{ pixels}}.

Physical check

Fine pixels can sample an optical line well, but they cannot recover spectral detail removed by the optical response.