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Distributed Brillouin sensing with sub-meter spatial resolution based on four-section pulse OM3G.3(OFC2013) Presenter: Heng Kong Date: 2013-4-9.

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Presentation on theme: "Distributed Brillouin sensing with sub-meter spatial resolution based on four-section pulse OM3G.3(OFC2013) Presenter: Heng Kong Date: 2013-4-9."— Presentation transcript:

1 Distributed Brillouin sensing with sub-meter spatial resolution based on four-section pulse OM3G.3(OFC2013) Presenter: Heng Kong Date: 2013-4-9

2 Outline Content Introduction Operation Principle Experimental results and discussion Conclusion Four-section pulse based Brillouin distributed fiber sensor sub-meter spatial resolution mitigate the secondary “echo” directly without extra measurement time and post-processing algorithm” State Key Laboratory of Information Photonics & Optical Communications (Beijing University of Posts and Telecommunications)

3 Background Rayleigh Scattering Raman Scattering Brillouin Scattering Fresnel Reflection Brillouin Scattering Spontaneous Brillouin Scattering Stimulated Brillouin Scattering

4 Introduction Distributed fiber sensors based on Brillouin optical time- domain analysis(BOTDA): ProblemsSolutionsDisadvantages Spatial resolution < 1m Pre-pulse, dark-pulse,π- phase-shift pulse Exits the secondary “echo” Secondary “echo”Differential pulse pair,π- phase-shift pulse pair The measurement time is twice longer Long measurement time Brillouin gain-profile tracing; deconvolution based method Need use post-processing algorithm

5 Operation Principle Fig.1. (a): dark pump pulse. T determines the spatial resolution; (b) four-section pump pulse. T1 determines the spatial resolution. (c) Probe traces vs. position. Blue trace: probe trace based on dark pulse technique; Red trace: probe trace based on four section pulse technique. Features: a)Higher spatial resolution than bright pulse; T determines the spatial resolution b)T1 acts as sensing pulse;T2 plays the role of mitigating the secondary “echo”; The longer T1, the longer T2 c)four-section pulse is better

6 Experimental results and discussion Fig. 2. Experimental setup. PC: polarization controller: EOM: electro-optic modulator; EDFA: Erbium-doped fiber amplifier; PD: photo-detector; PG: pulse generator. 25 ℃ 10.818GHz(10m) 70 ℃ 10.856GHz(50cm) 20dBm 1550nm 3kHz 1mW β:5ns,β’:10ns α:100mW β:1mW β’:120mW γ:100mW 50:50 700MHz 500MHz 1G/s

7 Experimental results and discussion Fig. 3. (a) The 3D-mapping of Brillouin gain versus both location and frequency shift with dark pulse based technique. (b) The 3D-mapping of Brillouin gain versus both location and frequency shift with four-section pulse based technique. Fig. 4. (a) Top view of 3D-mapping with dark pulse based technique. (b) Spectral gain curves at two typical locations with dark pulse based technique. (c) Top view of 3D-mapping with four-section pulse based technique. (d) Spectral gain curves at two typical locations with four-section pulse based technique. 观测到 BFS

8 Conclusion A novel Brillouin distributed fiber sensor based on four- section pulse: Theoretical analysis and experimental demonstration (10m long, 50cm spatial resolution) Mitigate the secondary “echo” phenomenon directly Hope it can help the development in future

9 Thank You ! More details: http://www.ofcnfoec.org/home/ http://front.sjtu.edu.cn/~llyi/waveguide


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