Interference from Thin Films — Question 2

Section 35-6 · Physics pages 5814–5815

Question 2 Two reflection phase reversals exchange the bright and dark thickness conditions A film of index nf = 1.50 lies between air (n0 = 1.00) and a substrate of index ns = 2.00. Light of vacuum wavelength 600 nm is incident normally. Treat reflected maxima and minima by the phase difference of the first two rays. n0 nf ns t 1.00 < 1.50 < 2.00 Schematic; labels, not drawing lengths, specify the data. (a) Identify both reflection phase shifts and find the least positive thickness for a reflected minimum. (b) Find the least positive thickness for a reflected maximum and state whether a phase minimum necessarily means zero reflectance.
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Question 2 - Solution Two reflection phase reversals exchange the bright and dark thickness conditions n0 nf ns t 1.00 < 1.50 < 2.00 (a) Method and calculation ϕ01 = π, ϕfs = π =⇒∆ϕr = 0; δ = 4πnft/λ0. δ = π =⇒tmin = λ0/(4nf) = 100 nm . (b) Interpretation and further calculation δ = 2π =⇒tmax,positive = λ0/(2nf) = 200 nm . Imin = ( √ I1 − √ I2)2 =⇒Imin = 0 only for equal interfering amplitudes . Physical check The relevant reflection contribution is the difference of the two phase shifts; two pi reversals cancel in the relative phase.

Question 2

Two reflection phase reversals exchange the bright and dark thickness conditions

A film of index nf=1.50n_f=1.50 lies between air (n0=1.00n_0=1.00) and a substrate of index ns=2.00n_s=2.00. Light of vacuum wavelength 600nm600\,\mathrm{nm} is incident normally. Treat reflected maxima and minima by the phase difference of the first two rays.

Diagram shown in the original SVG worksheet.

  1. Identify both reflection phase shifts and find the least positive thickness for a reflected minimum.

  2. Find the least positive thickness for a reflected maximum and state whether a phase minimum necessarily means zero reflectance.

Question 2 - Solution

Two reflection phase reversals exchange the bright and dark thickness conditions

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ϕ01=π,ϕfs=π⇒Δϕr=0;δ=4πnft/λ0.\phi_{01}=\pi,\quad\phi_{fs}=\pi\Longrightarrow\Delta\phi_r=0;\quad\delta=4\pi n_ft/\lambda_0.δ=π⇒tmin=λ0/(4nf)=100nm.\delta=\pi\Longrightarrow\boxed{t_{\mathrm{min}}=\lambda_0/(4n_f)=100\,\mathrm{nm}}.

(b) Interpretation and further calculation

δ=2π⇒tmax,positive=λ0/(2nf)=200nm.\delta=2\pi\Longrightarrow\boxed{t_{\mathrm{max,positive}}=\lambda_0/(2n_f)=200\,\mathrm{nm}}.Imin=(I1−I2)2⇒Imin=0only for equal interfering amplitudes.I_{\min}=(\sqrt{I_1}-\sqrt{I_2})^2\Longrightarrow\boxed{I_{\min}=0\ \text{only for equal interfering amplitudes}}.

Physical check

The relevant reflection contribution is the difference of the two phase shifts; two pi reversals cancel in the relative phase.