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Coherence (chapter 8) Coherence theory is the study of correlation that exist between different parts of a light field Two type of coherences: Temporal coherence: correlation between Spatial coherence: correlation between Temporal coherence can be measured with a Michelson interferometer Spatial coherence can be measured with a two-slit interferometer P. Piot, PHYS , NIU FA2018
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Michelson Interferometer
Case of a monochromatic plane wave Total intensity at the detector is Case of two wave packets? P. Piot, PHYS , NIU FA2018
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Michelson interferometer II
Consider two arbitrary waveforms the total field is The total intensity is then P. Piot, PHYS , NIU FA2018
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Degree of coherence function
Integrate previous equation over time And introduce the fluence The 3rd term is So that Use of Parseval’s theorem Degree of coherence function P. Piot, PHYS , NIU FA2018
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Example of a Gaussian wavepacket
Consider a Gaussian wavepacket Its power spectrum is The degree of coherence is given by So that P. Piot, PHYS , NIU FA2018
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Coherence time and fringe visibility
𝜏 𝑐 Cohrence time is defined as the amount of delay necessary to cause 𝛾(𝜏) to approach. A somewhat arbitrary definition is To the coherence time one can associate a coherence length The fringe visibility is defined as P. Piot, PHYS , NIU FA2018
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Fourier Spectroscopy The output signal of a Michelson interferometer for a pulsed signal If we take the Fourier transform we get So a measurement of the autocorrelation provides the spectrum of the signal. This is the essence of Fourier spectroscopy a widely used technique P. Piot, PHYS , NIU FA2018
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Spatial coherence Consider the double slits “spatial” interferometer and a point source This is similar to the Michelson interferometer except. Note theTaylor expansion 𝑑 1,2 𝑦 = 𝑦± ℎ 𝐷 2 1/2 ≃𝐷(1+ 𝑦± ℎ …) So the latter equation hold assuming 𝐷≫𝑦 and 𝐷≫ℎ. P. Piot, PHYS , NIU FA2018
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Case of an extended source
The fields are And the total field is found via Total intensity is P. Piot, PHYS , NIU FA2018
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Case of an extended source II
Assume the phases of emis- sion are random: The we get the time-averaged intensity Of the form P. Piot, PHYS , NIU FA2018
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