Michelson's Interferometer — Question 9

Section 35-7 · Physics pages 5848–5849

Question 9 Matching carrier phase does not necessarily match pulse arrival time In a Michelson interferometer, arm A contains a plate of thickness tA = 1.00 mm with phase index nA = 1.50 and group index ngA = 1.54. Arm B contains thickness tB of another material with nB = 1.60 and ngB = 1.62. Each plate replaces air on both passes; all other geometric paths match. Use air indices equal to 1 and c = 3.00 × 108 m/s. M1 M2 detector input A B Schematic; labels, not drawing lengths, specify the data. (a) Find tB for exact equality of excess carrier optical path. (b) Calculate the remaining group-delay difference A minus B and determine which pulse arrives later.
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Question 9 - Solution Matching carrier phase does not necessarily match pulse arrival time M1 M2 detector input A B (a) Method and calculation 2(nA −1)tA = 2(nB −1)tB =⇒tB = 0.50 0.60(1.00 mm) = 0.833333 mm . ∆Lcarrier = 2[0.50tA −0.60tB] = 0 . (b) Interpretation and further calculation ∆τg = 2 c[(ngA −1)tA −(ngB −1)tB] = 2 c [0.540 −0.516667] mm. ∆τg = +0.155556 ps; arm A arrives later . Physical check Broadband pulse overlap requires group-delay matching as well as carrier-phase alignment; the two materials have different dispersion.

Question 9

Matching carrier phase does not necessarily match pulse arrival time

In a Michelson interferometer, arm A contains a plate of thickness tA=1.00mmt_A=1.00\,\mathrm{mm} with phase index nA=1.50n_A=1.50 and group index ngA=1.54n_{gA}=1.54. Arm B contains thickness tBt_B of another material with nB=1.60n_B=1.60 and ngB=1.62n_{gB}=1.62. Each plate replaces air on both passes; all other geometric paths match. Use air indices equal to 1 and c=3.00×108m/sc=3.00\times10^8\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Find tBt_B for exact equality of excess carrier optical path.

  2. Calculate the remaining group-delay difference A minus B and determine which pulse arrives later.

Question 9 - Solution

Matching carrier phase does not necessarily match pulse arrival time

Diagram shown in the original SVG worksheet.

(a) Method and calculation

2(nA−1)tA=2(nB−1)tB⇒tB=0.500.60(1.00mm)=0.833333mm.2(n_A-1)t_A=2(n_B-1)t_B\Longrightarrow\boxed{t_B=\frac{0.50}{0.60}(1.00\,\mathrm{mm})=0.833333\,\mathrm{mm}}.Δℒcarrier=2[0.50tA−0.60tB]=0.\boxed{\Delta\mathcal L_{\mathrm{carrier}}=2[0.50t_A-0.60t_B]=0}.

(b) Interpretation and further calculation

Δτg=2c[(ngA−1)tA−(ngB−1)tB]=2c[0.540−0.516667]mm.\Delta\tau_g=\frac2c[(n_{gA}-1)t_A-(n_{gB}-1)t_B]=\frac2c\left[0.540-0.516667\right]\mathrm{mm}.Δτg=+0.155556ps;arm A arrives later.\boxed{\Delta\tau_g=+0.155556\,\mathrm{ps};\quad\text{arm A arrives later}}.

Physical check

Broadband pulse overlap requires group-delay matching as well as carrier-phase alignment; the two materials have different dispersion.