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{ Abstract / Résumé }
Chapter 1
Chapter 2
{ 3.1 }
{ 3.2 }
{ 3.3.1 }
{ 3.3.2 }
3.3.3.a : Source effect (Bandwidth)
Ph.D.  /  { Web Version }  /  Chapter 3  /  3.3  /  { 3.3.3 }  /  3.3.3.b : Source effect (Detuning)
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Physics Diploma
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Chapter 4
Chapter 5
Chapter 6
Chapter 7
Chapter 8
Appendix
Other parts
{ 3.4 }
{ 3.5 }
3.6
3.7

3.3        Calculated FBG spectral and impulse responses

3.3.3       Source effect

b)   Source detuning effect

The influence of the detuning wavelength between the FBG and the broadband source central wavelength has been studied for a 40 nm bandwidth source. The results are shown in Fig. 3-23 for a detuning of 0, 10, 30 and 50 nm, respectively. The impulse responses for a detuning smaller than 10 nm are very close to the case without detuning. For a more important detuning, the impulse amplitude drops consistently due to the reduced overlap between the FBG and the source. Another effect also appears : for high detuning, the amplitude signal at the grating input and output presents an peak due to the refractive index step that acts like a broadband mirror. This is presented in the zoomed view of the grating output in Fig. 3-23 (the curves has been shifted in the OPLD axis for clarity). The phase difference shows a smoothing effect, that is the p-shifts are spread over an OPLD range proportional to the detuning.

Fig. 3-23 Source detuning effect on the complex impulse response amplitude (top) and phase difference (bottom) for a 10 mm homogeneous grating with 2×10-4 refractive index modulation; 0 nm (solid lines), 10 nm (dashed lines), 30 nm (dashed-dotted lines) and 50 nm (dotted lines) detuning values are considered



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Path :  www.lphg.ch Ph.D. { Web Version } Chapter 3 3.3 { 3.3.3 } 3.3.3.b
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