3.4.2 : Layer thickness Activate Navigation Menu 3.4.4 : Reduction of the Gibb's effect

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CV

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Ph.D.

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{ Web Version }

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Table of Contents

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{ Abstract / Résumé }

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Chapter 1

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Chapter 2

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Chapter 3

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{ 3.1 }

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{ 3.2 }

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3.3

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{ 3.4 }

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3.4.1

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3.4.2

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3.4.3

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3.4.4

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3.4.5

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3.4.6

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{ 3.5 }

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3.6

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3.7

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Chapter 4

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Chapter 5

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Chapter 6

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Chapter 7

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Chapter 8

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Appendix

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Other parts

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Post-Doc

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MBI

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Physics Diploma

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Photos

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3.4.1 : Reconstruction limits

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3.4.2 : Layer thickness

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3.4.3 : Number of points

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3.4.4 : Reduction of the Gibb's effect

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3.4.5 : Reconstruction from the complex spectral response

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3.4.6 : Reconstruction from the complex impulse response

3.4        Reconstruction examples

3.4.3       Number of points

The choice of the number of spectral points M required for the reconstruction process by layer-peeling is not absolute but depends on the number of layers N (and is then inversely related to the layer thickness). Fig. 3-27 presents the reconstructions of FBG1 performed with a 3 mm-layer thickness and a ratio M/N of 1, 2, 5 and 10, respectively. The reconstruction is poor for M = N and fairly good for M = 2N. For M/N higher than 5 or ten, the results are very close. For very strong gratings, a ratio increase to 30 or 50 improves the reconstruction, but not in a significantly way (Fig. 3-24).

Fig. 3-27 Reconstructed coupling coefficient amplitude (top) and local Bragg wavelength (bottom) for the FBG1 performed with layers thickness of 3 mm and different ratio M/N : 10 for the solid lines, 5 for the dashed lines, 2 for the dashed-dotted lines and 1 for the dotted lines; the curves are translated for clarity



3.4.2 : Layer thickness Activate Navigation Menu 3.4.4 : Reduction of the Gibb's effect