Diffraction by a Double Slit — Question 7

Section 36-6 · Physics pages 5964–5965

Question 7 Polarization mismatch fills interference minima but preserves envelope zeros Equal finite slits have individual intensity Is sinc2 β. Their transmitted fields are linearly polarized at angle χ = 60◦to each other and have phase difference 2α. A polarization-insensitive detector measures their sum. d P slit width a Schematic; labels, not drawing lengths, specify the data. (a) Derive the intensity and local visibility as phase is scanned at a fixed nonzero envelope value. (b) Find the maximum and minimum levels in units of Is sinc2 β, and evaluate the intensity at an envelope zero.
Show solutionHide solution
Question 7 - Solution Polarization mismatch fills interference minima but preserves envelope zeros d P slit width a (a) Method and calculation I = 2Is sinc2 β[1 + cos χ cos(2α)] . V = | cos χ| = 1/2 . (b) Interpretation and further calculation Imax = 3Is sinc2 β, Imin = Is sinc2 β . sinc β = 0 =⇒I = 0 for every relative phase . Physical check Polarization overlap controls the cross term, whereas an individual-slit zero removes both fields before they can interfere.

Question 7

Polarization mismatch fills interference minima but preserves envelope zeros

Equal finite slits have individual intensity Issinc⁡2βI_s\operatorname{sinc}^2\beta. Their transmitted fields are linearly polarized at angle χ=60∘\chi=60^\circ to each other and have phase difference 2α2\alpha. A polarization-insensitive detector measures their sum.

Diagram shown in the original SVG worksheet.

  1. Derive the intensity and local visibility as phase is scanned at a fixed nonzero envelope value.

  2. Find the maximum and minimum levels in units of Issinc⁡2βI_s\operatorname{sinc}^2\beta, and evaluate the intensity at an envelope zero.

Question 7 - Solution

Polarization mismatch fills interference minima but preserves envelope zeros

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I=2Issinc⁡2β[1+cos⁡χcos⁡(2α)].\boxed{I=2I_s\operatorname{sinc}^2\beta[1+\cos\chi\cos(2\alpha)]}.V=|cos⁡χ|=1/2.\boxed{V=|\cos\chi|=1/2}.

(b) Interpretation and further calculation

Imax=3Issinc⁡2β,Imin=Issinc⁡2β.\boxed{I_{\max}=3I_s\operatorname{sinc}^2\beta,\quad I_{\min}=I_s\operatorname{sinc}^2\beta}.sinc⁡β=0⇒I=0for every relative phase.\operatorname{sinc}\beta=0\Longrightarrow\boxed{I=0\ \text{for every relative phase}}.

Physical check

Polarization overlap controls the cross term, whereas an individual-slit zero removes both fields before they can interfere.