B.2 : Ray optic concatenation of lenses Activate Navigation Menu C.1 : Scalar wave approximation

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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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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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{ Appendix A }

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{ Appendix B }

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B.1

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B.2

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B.3

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{ Appendix C }

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{ Appendix D }

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{ Appendix E }

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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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B.1 : Introduction

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B.2 : Ray optic concatenation of lenses

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B.3 : Modified phase mask technique

B.3      Modified phase mask technique

From Fig. B-1 we see that r0 = ¥, s0 = fx and L0 = 2h0. We then obtain






(B-4)


The distances L and L+DL are given by




(B-5)


The relative Bragg wavelength change lb/lb,0 and the absolute Bragg wavelength shift Dlb correspond to




(B-6)


where he magnification is close to 1 and then the |.| is omitted. We have realized a set-up with the following parameters :

-         fx  = 100 mm

-         fv = -20 mm

-         d1 = 32 mm

-         d2 = 13 mm

We observe that for these parameters, the beam width is identical at the phase mask location to the beam size at the entrance (L = h0). For an initial Bragg wavelength of 1550 nm, the parameter a has a value of 24.2 m-1. For the fiber touching the phase mask, the distance d3 = 62.5 mm (fiber radius) and then the Bragg wavelength shift is 2.35 nm as can be seen in Fig. B-4.

Fig. B-4 Wavelength shift for the realized set-up and a phase mask for FBG writing at 1550 nm



B.2 : Ray optic concatenation of lenses Activate Navigation Menu C.1 : Scalar wave approximation