Diffraction Gratings — Question 5

Section 36-7 · Physics pages 5980–5981

Question 5 A one-third open grating suppresses every third nonzero principal order An ideal scalar amplitude grating has transparent width a = d/3 in each period. Its normalized Fourier coefficient is cm = f sinc(πmf), with open fraction f = a/d. In this model the power fraction in order m is ηm = |cm|2. Ignore obliquity corrections. d N illuminated slits a = d/3 Schematic; labels, not drawing lengths, specify the data. (a) Find the missing principal orders. (b) Calculate the zero-order and each first-order power fraction relative to incident power.
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Question 5 - Solution A one-third open grating suppresses every third nonzero principal order d N illuminated slits a = d/3 (a) Method and calculation πmf = mπ/3; sin(mπ/3) = 0 for m = 3p, p̸ = 0. m = ±3, ±6, . . . are suppressed . (b) Interpretation and further calculation η0 = f2 = 1/9 = 0.111111 . η+1 = η−1 = [sin(π/3) π ]2 = 3 4π2 = 0.0759909 . Physical check An open fraction of one third does not put one third of the incident power into the zero order; the transmitted field is distributed among orders.

Question 5

A one-third open grating suppresses every third nonzero principal order

An ideal scalar amplitude grating has transparent width a=d/3a=d/3 in each period. Its normalized Fourier coefficient is cm=fsinc⁡(πmf)c_m=f\operatorname{sinc}(\pi mf), with open fraction f=a/df=a/d. In this model the power fraction in order m is ηm=|cm|2\eta_m=|c_m|^2. Ignore obliquity corrections.

Diagram shown in the original SVG worksheet.

  1. Find the missing principal orders.

  2. Calculate the zero-order and each first-order power fraction relative to incident power.

Question 5 - Solution

A one-third open grating suppresses every third nonzero principal order

Diagram shown in the original SVG worksheet.

(a) Method and calculation

πmf=mπ/3;sin⁡(mπ/3)=0form=3p,p≠0.\pi mf=m\pi/3;\quad\sin(m\pi/3)=0\ \text{for}\ m=3p,\ p\ne0.m=±3,±6,…are suppressed.\boxed{m=\pm3,\pm6,\ldots\ \text{are suppressed}}.

(b) Interpretation and further calculation

η0=f2=1/9=0.111111.\boxed{\eta_0=f^2=1/9=0.111111}.η+1=η−1=[sin⁡(π/3)π]2=34π2=0.0759909.\boxed{\eta_{+1}=\eta_{-1}=\left[\frac{\sin(\pi/3)}\pi\right]^2=\frac3{4\pi^2}=0.0759909}.

Physical check

An open fraction of one third does not put one third of the incident power into the zero order; the transmitted field is distributed among orders.