1987
DOI: 10.1364/josaa.4.000494
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Temporal coherence properties of a dispersively propagating beam in a fiber-optic interferometer

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Cited by 14 publications
(6 citation statements)
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“…Low-coherence light sources are usually used to measure the group delay dispersion with sub-picosecond resolution. The temporal coherence degrades when the interference involves two waves with different group velocity dispersions (GVDs) [7,8,9,10]. The influence is on the measurement accuracies of DGD and chromatic dispersion, since the curve shape of the degree of coherence, jj, with respect to the interference broadens as the GVD and fiber length increase.…”
Section: Introductionmentioning
confidence: 99%
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“…Low-coherence light sources are usually used to measure the group delay dispersion with sub-picosecond resolution. The temporal coherence degrades when the interference involves two waves with different group velocity dispersions (GVDs) [7,8,9,10]. The influence is on the measurement accuracies of DGD and chromatic dispersion, since the curve shape of the degree of coherence, jj, with respect to the interference broadens as the GVD and fiber length increase.…”
Section: Introductionmentioning
confidence: 99%
“…As was introduced in Ref. [7], Hamilton et al [11] analyzed the coherence properties of a dispersively propagating wave such as electrons or neutrons in vacuo, or light in a medium, and discussed the observation of its spatial and temporal coherence properties by means of a two-beam interferometer. A numerical dispersion compensation technique has been also presented for optical coherence tomography [12].…”
Section: Introductionmentioning
confidence: 99%
“…Scanning Michelson white light interferometers can be used to obtain such distributed polarization cross-talk measurements [3,5]. Unfortunately, as the length of the fiber under test (FUT) increases, the measured cross-talk peaks will be broadened due to birefringence dispersion [6], resulting in reduced spatial resolution and degraded crosstalk amplitude measurement accuracies [7][8][9] for PM fibers with a length exceeding a few hundred meters.…”
mentioning
confidence: 99%
“…The envelope of a measured cross-talk peak (the interference peak) is influenced by the SLED's spectral distribution and the birefringence dispersion ΔD of the PM fiber [6][7][8]. Assume that the SLED has a Gaussian spectral shape; the cross-talk envelope (the degree of coherence) γ can be derived as the function of birefringence dispersion ΔD and the distance Z of cross-talk point measured from the output [6][7][8]:…”
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confidence: 99%
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