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CV
Table of Contents
{ Abstract / Résumé }
Chapter 1
Chapter 2
Chapter 3
Chapter 4
Chapter 5
Chapter 6
Chapter 7
Chapter 8
{ Appendix A }
B.1 : Introduction
B.2 : Ray optic concatenation of lenses
Ph.D.  /  { Web Version }  /  Appendix  /  { Appendix B }  /  B.3 : Modified phase mask technique
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{ Appendix C }
{ Appendix D }
{ Appendix E }

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



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