A subscription to JoVE is required to view this content. Sign in or start your free trial.
A protocol for Brillouin optical time-domain analyzers based on gain spectrum engineering is presented. Enhancements in the sensing performance, including sensing range and measurand resolution are achieved and the excess Brillouin intensity noise is studied. The protocol introduces a new way to enhance distributed Brillouin sensing performance.
Demonstrated is a unique method for sensing performance enhancement in Brillouin optical time-domain analyzers (BOTDA). A Brillouin gain spectrum (BGS) is superimposed with two symmetric Brillouin loss spectra (BLS). This leads to a complex engineered spectrum shape that is more resistant to the sensing system noise. Instead of only one pump and probe interaction as in the conventional BOTDA setup, three optical probe waves are exploited, with one probe located in the BGS and the other two symmetrically in the BLS. Due to the resistance and insensitivity of the engineered spectrum shape to the noise, the sensing performance is enhanced by 60% and the measurand resolution is doubled.
Distributed fiber sensing (DFS) is a unique mechanism that employs a whole fiber as a sensing medium. It has attracted a lot of interest due to the low fiber loss; small size; and the ability to be easily embedded in various structures, such as dams, bridges, and buildings, to perform environment surveillance as an artificial nerve system. In comparison to applying numerous traditional point sensors, such as fiber Bragg gratings (FBG), it provides a more efficient and cost-effective solution in a wide range of large-scale sensing tasks, such as infrastructure and structural health monitoring1.
Current distributed sen....
1. Selecting optimized parameters for the spectrum engineering via simulation
Figure 3 shows the simulation results. Points with η < 1 in Figure 3A indicate a smaller frequency error (higher measurand resolution) with the engineered BGS. The lower the value was, the bigger the advantage. The minimum ratio was at m = 1, indicating that a multiprobe instead of multipump scheme can be carried out (see Discussion). Figure 3B
The most critical step during the experiment is the equalization of the three probe powers so that m = 1 and symmetry between the two Brillouin loss spectra is achieved. Besides the separate power check using the power meter at Cir port 2, as presented in steps 4.9 and 4.10, the power equalization can be more precisely checked in the digitizer. By setting the RF 1 frequency to ~11 GHz (the fiber BFS) and switching off EDFA 3, the conventional trace with the peak gain can be recorded in the digitizer (trace I). T.......
Cheng Feng wishes to acknowledge the financial support from German Research Foundation (SCHN 716/13-1, 716/15-2, 716/18-1, 716/26-1) and Niedersächsisches Vorab (NL-4 Project "QUANOMET").
....Name | Company | Catalog Number | Comments |
Current controller for laser diode | ILX Lightwave | LDX3220 | |
Digitizer | Acqiris SA | U5309A-1039 | |
Erbium doped fiber amplifier 1 | Photop | PTEDFA-A-PA-C-SCH-15 | |
Erbium doped fiber amplifier 2 | LiComm | OFA-TCH | |
Erbium doped fiber amplifier 3 | Calmar Optcom | AMP-ST30 | |
Erbium doped fiber amplifier 4 | Photop | PTEDFA-A-PA-C-SCH-15 | |
Fiber Bragg grating 1 | Advanced Optics Solutions | T-FBG | |
Fiber Bragg grating 2 | Advanced Optics Solutions | T-FBG | |
Fiber under test | ofs | ||
Isolator | General Photonics | S-15-NTSS | |
Laser diode | 3SP Group | A1905 LMI | |
Mach-Zehnder modulator 1 | Avanex | IM10 | |
Mach-Zehnder modulator 2 | Avanex | IM10 | |
Mach-Zehnder modulator 3 | Avanex | IM10 | |
Nanosecond driving board for semiconductor optical amplifier | Highland Technology | T160-9 (28A160-9C) | |
Optical coupler 10:90 | Newport | Benchtop coupler/WDM | |
Optical coupler 50:50 | Newport | Benchtop coupler/WDM | |
Optical spectrum analyzer | Hewlett Packard | 86145A | |
Optical switch 1 | JDSU | SN12-1075NC | |
Photodiode | Thorlabs | D400FC | |
Polarization scrambler | General Photonics | PSY-101 | |
Pulase generator | Hewlett Packard | 8082A | |
Radio function generator 1 | Anritsu | MG3692C | |
Radio function generator 2 | Agilent Technology | E8257D | |
Radio function generator 3 | HTM | T2100 | |
Semiconductor optical amplifier | Thorlabs | SOA1013SXS | |
Temperature controller for laser diode | ILX Lightwave | LDT5948 | |
Temperature controller for semiconductor optical amplifier | Tektronix | TED200 | |
Variable optical attenuator | JDSU | mVOA-A1 | With optical switch function |
This article has been published
Video Coming Soon
ABOUT JoVE
Copyright © 2024 MyJoVE Corporation. All rights reserved