3.1.5 : Causal T-matrix method Activate Navigation Menu 3.2.2 : Discrete Layer-peeling

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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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3.2.1

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3.2.2

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3.2.3

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3.3

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{ 3.4 }

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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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3.2.1 : Overview of reconstruction methods

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3.2.2 : Discrete Layer-peeling

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3.2.3 : Reconstructed FBG interpretation

3.2        FBG synthesis and reconstruction

This section presents an overview of the different methods used to retrieve the local parameters of a grating. A large emphasis has been given to the layer-peeling method, which has been employed in this work.

3.2.1        Overview of reconstruction methods

The retrieval of the grating parameters distribution from the grating spectral response has been widely studied. Several papers have been published where only the spectral amplitude or phase was exploited. In this case, the grating distributions needs to be monotonic [3-7, 3-8] or a priori assumption needs to be postulated (for example a gradient direction) [3-9]. As a consequence, only one parameter can be retrieved. For weak gratings, the knowledge of the intensity and the phase of the spectral response permits to reconstruct the grating profile via a Fourier Transform [3-2, 3-10]; for strong gratings, a backscattering technique is instead necessary [3-11, 3-12]. The layer-peeling technique discussed hereafter is a backscattering technique, which is highly efficient and not very sensitive to the measurement noise, when applied to the complex impulse response. Some methods use an iterative process where at each step a theoretical grating profile and its reflection or phase spectrum are generated and compared with a measured spectrum [3-13 to 3-16].



3.1.5 : Causal T-matrix method Activate Navigation Menu 3.2.2 : Discrete Layer-peeling