Coherence — Question 10

Section 35-4 · Physics pages 5790–5791

Question 10 Pulse overlap limits time-integrated interference contrast Two equal-energy, identically polarized coherent pulses have rectangular field envelopes of duration T. Their relative arrival delay is τ and their adjustable carrier phase is δ. The detector integrates over both entire pulses. Each isolated pulse deposits energy U, and the field amplitude is constant during its pulse. t envelope τ Schematic; labels, not drawing lengths, specify the data. (a) Derive the integrated energy as a function of phase and delay for |τ| < T. (b) Find the visibility for τ = 0.30T and state what happens for |τ| ≥T.
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Question 10 - Solution Pulse overlap limits time-integrated interference contrast t envelope τ (a) Method and calculation Toverlap = T −|τ|, ∫ E1E2 dt ∝(T −|τ|) cos δ. E = 2U [ 1 + ( 1 −|τ| T ) cos δ ] , V = 1 −|τ|/T . (b) Interpretation and further calculation τ = 0.30T =⇒V = 0.70 . |τ| ≥T : Toverlap = 0 =⇒E = 2U, V = 0 . Physical check Mutual carrier coherence alone is insufficient for ordinary intensity interference when the fields never overlap in time at the detector.

Question 10

Pulse overlap limits time-integrated interference contrast

Two equal-energy, identically polarized coherent pulses have rectangular field envelopes of duration T. Their relative arrival delay is τ\tau and their adjustable carrier phase is δ\delta. The detector integrates over both entire pulses. Each isolated pulse deposits energy U, and the field amplitude is constant during its pulse.

Diagram shown in the original SVG worksheet.

  1. Derive the integrated energy as a function of phase and delay for |τ|<T|\tau|<T.

  2. Find the visibility for τ=0.30T\tau=0.30T and state what happens for |τ|≥T|\tau|\geq T.

Question 10 - Solution

Pulse overlap limits time-integrated interference contrast

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Toverlap=T−|τ|,∫E1E2dt∝(T−|τ|)cos⁡δ.T_{\mathrm{overlap}}=T-|\tau|,\quad\int E_1E_2\,dt\ \propto\ (T-|\tau|)\cos\delta.ℰ=2U[1+(1−|τ|T)cosδ],V=1−|τ|/T.\boxed{\mathcal E=2U\left[1+\left(1-\frac{|\tau|}{T}\right)\cos\delta\right],\quad V=1-|\tau|/T}.

(b) Interpretation and further calculation

τ=0.30T⇒V=0.70.\tau=0.30T\Longrightarrow\boxed{V=0.70}.|τ|≥T:Toverlap=0⇒ℰ=2U,V=0.|\tau|\geq T:\quad T_{\mathrm{overlap}}=0\Longrightarrow\boxed{\mathcal E=2U,\quad V=0}.

Physical check

Mutual carrier coherence alone is insufficient for ordinary intensity interference when the fields never overlap in time at the detector.