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Table of Contents
{ Abstract / Résumé }
Chapter 1
Chapter 2
Chapter 3
4.1
{ 4.2 }
4.3.1 : Time multiplexing OLCR design
4.3.2 : Measurement principle
4.3.3 : Balanced detection scheme
4.3.4 : Polarization effects
4.3.5 : Wavelength multiplexing OLCR design
4.3.6 : Discussion on the different OLCR designs
Ph.D.  /  { Web Version }  /  Chapter 4  /  4.3  /  4.3.7 : Time multiplexing design in OFDR use
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Chapter 5
Chapter 6
Chapter 7
Chapter 8
Appendix
Other parts
{ 4.4 }
{ 4.5 }
4.6
4.7
4.3.8 : Transmission impulse response OLCR set-up

4.3        New OLCR set-ups

4.3.7       Time multiplexing design in OFDR use

The time multiplexing design OLCR has also been used to measure directly the complex spectral response of FBGs. To achieve this, the mirror is placed at a position corresponding to an inner point of the grating in order to have a strong low coherence signal. Instead of moving the mirror to scan the OPLD, the light frequency is scanned by the tunable laser. The low coherent signal phase is used to compensate the phase drifts. This measurement method is known as optical frequency division reflectometry (OFDR). The obtained complex signal corresponds to the complex reflection amplitude r(n) and not to the reflection intensity. For this reason, the dynamic range in dB is twice the one obtained with a direct intensity measurement. The dynamic range is nevertheless limited by the spontaneous light emission of the laser source. For the tunable laser we have used, the spontaneous light emission is under -60 dB. This dynamic limitation can be overcome for an amplitude measurement by placing the mirror at a position where the low coherence signal is canceled as the same will occur with the spontaneous part of the laser light, but the phase signal is lost in this case



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Path :  www.lphg.ch Ph.D. { Web Version } Chapter 4 4.3 4.3.7
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