Light as a Wave — Question 2

Section 35-1 · Physics pages 5714–5715

Question 2 A layered arm is balanced by changing a different material An interferometer replaces tA = 20 µm of air in arm A by material nA = 1.40. Arm B contains a variable thickness tB of material nB = 1.60, also replacing air. The remaining air paths give equal total geometric lengths. Ignore reflections. S P path 1 path 2 nA, tA nB, tB Schematic; labels, not drawing lengths, specify the data. (a) Find the positive thickness that gives equal optical paths without an integer-order ambiguity. (b) For vacuum wavelength 640 nm, find the phase error if arm B is made 0.20 µm too thick; define phase difference as B minus A.
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Question 2 - Solution A layered arm is balanced by changing a different material S P path 1 path 2 nA, tA nB, tB (a) Method and calculation LB −LA = (nB −1)tB −(nA −1)tA. ∆L = 0 =⇒tB = 0.40 0.60(20) = 13.333 µm . (b) Interpretation and further calculation δL = 0.60(0.20 µm) = 0.120 µm. δϕ = 2π0.120 0.640 = 0.375π rad ≃1.178 rad . Physical check The index contrast with the displaced air, rather than the material index alone, controls the compensation.

Question 2

A layered arm is balanced by changing a different material

An interferometer replaces tA=20μmt_A=20\,\mu\mathrm m of air in arm A by material nA=1.40n_A=1.40. Arm B contains a variable thickness tBt_B of material nB=1.60n_B=1.60, also replacing air. The remaining air paths give equal total geometric lengths. Ignore reflections.

Diagram shown in the original SVG worksheet.

  1. Find the positive thickness that gives equal optical paths without an integer-order ambiguity.

  2. For vacuum wavelength 640nm640\,\mathrm{nm}, find the phase error if arm B is made 0.20μm0.20\,\mu\mathrm m too thick; define phase difference as B minus A.

Question 2 - Solution

A layered arm is balanced by changing a different material

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ℒB−ℒA=(nB−1)tB−(nA−1)tA.\mathcal L_B-\mathcal L_A=(n_B-1)t_B-(n_A-1)t_A.Δℒ=0⇒tB=0.400.60(20)=13.333μm.\Delta\mathcal L=0\Longrightarrow\boxed{t_B=\frac{0.40}{0.60}(20)=13.333\,\mu\mathrm m}.

(b) Interpretation and further calculation

δℒ=0.60(0.20μm)=0.120μm.\delta\mathcal L=0.60(0.20\,\mu\mathrm m)=0.120\,\mu\mathrm m.δϕ=2π0.1200.640=0.375πrad≃1.178rad.\boxed{\delta\phi=2\pi\frac{0.120}{0.640}=0.375\pi\ \mathrm{rad}\simeq1.178\,\mathrm{rad}}.

Physical check

The index contrast with the displaced air, rather than the material index alone, controls the compensation.