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Table of Contents
{ Abstract / Résumé }
Chapter 1
Chapter 2
Chapter 3
4.1 : Methods for measuring the complex impulse response of a grating
{ 4.2 : OLCR measurement of the complex impulse response }
4.3 : New OLCR set-ups
{ 4.4 : Reconstruction process }
{ 4.5 : Reconstructed FBG }
Ph.D.  /  { Web Version }  /  Chapter 4  /  4.6 : Summary
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Chapter 5
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Chapter 7
Chapter 8
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4.7 : References

4.6        Summary

We have shown that for a wavelength bandwidth where the fiber dispersion is negligible, the complex OLCR response of a FBG corresponds to the convolution of the complex impulse response of the grating with the degree of coherence of the light source. We have also shown that the grating impulse response is less directly connected to the OLCR response in the case where the dispersion effects are not negligible. Nevertheless, it is experimentally or mathematically possible to retrieve the complex impulse response in this case.

We have detailed the new developed OLCR set-ups, explained the measurement method, the apparatus performances and the limitations. This instrument measures the amplitude and the phase information of the FBG. The main results concerns the time-multiplexing OLCR set-up that exhibits a noise level of -120 dB for optical fiber devices (limited by the Rayleigh back-scattering) and a large range of allowed OPLD resolution due to the phase difference measurement method.

The reconstruction process from the OLCR measurement to the complex coupling coefficient has been presented and the reconstruction of different FBGs has been shown. The main results are an axial resolution of 20 mm and a maximal absolute error of the amplitude and the phase of 5 % calculated by comparison between the reconstructions conducted from both side of the FBG. The reconstruction of a FBG that exhibits loss has also been reconstructed using the modified layer-peeling method and a good matching between the reconstructions from both sides is observed.



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