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CN109084883A - Based on phase-BOTDR optical fiber distributed type Brillouin's vibrating sensing measurement method - Google Patents

Based on phase-BOTDR optical fiber distributed type Brillouin's vibrating sensing measurement method Download PDF

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Publication number
CN109084883A
CN109084883A CN201810904352.8A CN201810904352A CN109084883A CN 109084883 A CN109084883 A CN 109084883A CN 201810904352 A CN201810904352 A CN 201810904352A CN 109084883 A CN109084883 A CN 109084883A
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phase
brillouin
light
variation
zehnder interferometer
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姜海明
赵蕊月
张令春
谢康
刘晨
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Hefei University of Technology
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Hefei University of Technology
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H9/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
    • G01H9/004Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means using fibre optic sensors

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Optical Transform (AREA)

Abstract

本发明提出了一种基于相位‑BOTDR布里渊光纤分布式振动传感测量方法,光源发出的连续光经脉冲调制器调制成脉冲光,通过掺铒光纤放大器进行放大,放大后的脉冲光经光环行器进入单模传感光纤,发生振动变化位置处的后向布里渊散射光再经光环形器进入光纤布拉格光栅,滤除噪声,布里渊散射光经非平衡马赫泽德干涉仪发生干涉,输出的三路光被光电探测器接收后由数据采集处理系统进行处理。利用非平衡马赫泽德干涉仪结构,将后向散射的布里渊频移变化量转化为干涉光输出相位的变化,采用相位解调方法,利用反三角函数法解调相位,得到布里渊频移变化,从而实现光纤动态应变的测量,比微分交叉相乘方法得到的相位精确度高。

The present invention proposes a Brillouin optical fiber distributed vibration sensing measurement method based on phase-BOTDR. The continuous light emitted by the light source is modulated into pulsed light by a pulse modulator, amplified by an erbium-doped optical fiber amplifier, and the amplified pulsed light is passed through The optical circulator enters the single-mode sensing fiber, and the Brillouin scattered light at the position where the vibration changes occurs enters the fiber Bragg grating through the optical circulator to filter out noise, and the Brillouin scattered light passes through the unbalanced Mach-Zehnder interferometer Interference occurs, and the output three-way light is received by the photodetector and then processed by the data acquisition and processing system. Using the non-equilibrium Mach-Zehnder interferometer structure, the Brillouin frequency shift change of the backscattering is converted into the change of the output phase of the interfering light, and the phase demodulation method is used to demodulate the phase using the inverse trigonometric function method to obtain the Brillouin The frequency shift changes, so as to realize the measurement of the dynamic strain of the optical fiber, and the phase accuracy obtained by the differential cross multiplication method is higher.

Description

Based on phase-BOTDR optical fiber distributed type Brillouin's vibrating sensing measurement method
Technical field
It is specifically a kind of based on phase-BOTDR Brillouin fiber optic point the present invention relates to Distributed Optical Fiber Sensing Techniques field The measurement of formula cloth vibrating sensing.
Background technique
Distributed fiber optic sensing is widely used in urban construction Bridge, railway monitoring, rocket propulsion system and oil well inspection Survey etc., it mainly uses the light scattering theory in optical fiber, including Rayleigh scattering, Raman scattering and Brillouin scattering.Mesh In preceding domestic and international optical fiber sensing system, the Distributed Optical Fiber Sensing Techniques based on Rayleigh scattering are usually used in breakpoints of optical fiber and decaying is special The qualitative detection of sign also has been reported that and carries out strain measurement (bibliography Masoudi A, Belal to Rayleigh scattering using after optical fiber M,Newson T P.A distributed optical fibre dynamic strain sensor based on phase-OTDR[J].Measurement Science&Technology,2013,24(8):085204.);Raman scattering is main It is measured for temperature sensing;Brillouin scattering can be used for the detection of remote temperature strain and vibration, be current high-precision sensing The big hot spot of the one of fields of measurement.
Realize remote, high spatial resolution, high sensitivity Fibre Optical Sensor, main limited resource includes: excessive arteries and veins The nonlinear effect for rushing power generation influences;Dynamic range caused by pulse width changes can not get both with resolution ratio;It is faint to dissipate Penetrate the detection of signal and the processing of Dynamic Signal etc..Overcome the challenge encountered in high-precision Distributed Optical Fiber Sensing Techniques, Meet the actual demand for solving national economy and the people's livelihood.High-precision distributed sensing technology based on Brillouin scattering mainly has Brillouin light Time-domain analysis half-light pulse technique, Brillouin light domain of dependence analytical technology and Brillouin light frequency-domain analysis technology.About dynamically answering The measurement of change is had been reported that before using phase sensitive optical time domain detection technique (bibliography Zhang X, Sun Z, Shan Y, et al.A high performance distributed optical fiber sensor based onΦ-OTDR for Dynamic strain measurement [J] .IEEE Photonics Journal, 2017, PP (99): 1-1.), Brillouin Phase-shift measurement and Brillouin's dynamic raster combined technology (bibliography Bergman A, Langer T, Tur M.Phase- based,high spatial resolution and distributed,static and dynamic strain sensing using Brillouin dynamic gratings in optical fibers.[J].Optics Express,2017,25(5):5376.).It is moved herein using based on phase sensitive Brillouin light time domain reflection technology State stress measurement is obtained Brillouin shift variation, realized using phase demodulating method using antitrigonometric function method demodulation phase Fiber-optic vibration measurement.
Summary of the invention
The invention proposes a kind of phase demodulation algorithms that strain is surveyed based on spontaneous brillouin scattering, to realize distributed light The dynamic strain measurement of phase sensitive in fibre sensing.
In order to achieve the above object, the technical scheme adopted by the invention is as follows:
One kind being based on phase-BOTDR Brillouin fiber optic distribution vibrating sensing measurement method, includes that distributed Feedback swashs Light source, Polarization Controller, pulse-modulator, erbium-doped fiber amplifier, optical circulator, single mode sensor fibre, optical fiber Bragg light Grid, non-equilibrium Mach Zehnder interferometer, photodetector and data acquisition processing system, the distributed feedback laser source hair Continuous light out is successively modulated into pulsed light through Polarization Controller, pulse-modulator, is amplified by erbium-doped fiber amplifier, Amplified pulsed light enters single mode sensor fibre through optical circulator, and the backward Brillouin scattering light at vibration variation occurs and passes through again Optical circulator enters fiber bragg grating, and Brillouin scattering is interfered through non-equilibrium Mach Zehnder interferometer, output Three road light are handled after being received by a photoelectric detector by data acquisition processing system, and non-equilibrium Mach Zehnder interferometer knot is utilized Structure converts the Brillouin shift variable quantity of back scattering to the variation of interference light output phase, according to different moments phase Variation demodulates Brillouin shift variable quantity, and then obtains the variation of the vibration along sensor fibre.
Using non-equilibrium Mach Zehnder interferometer structure, interference light is converted by the Brillouin shift variable quantity of back scattering The variation of phase is obtained Brillouin shift variation, realized using phase demodulating method using antitrigonometric function method demodulation phase Fiber-optic vibration measurement, the specific steps are as follows:
A. optical signal is acquired, three tunnel output optical signals are detected by photoelectric detector, backward Brillouin scattering light is by non- The three road light exported after the interference of balanced Mach Zehnder interferometer respectively indicate are as follows:
In above formula, I0For Brillouin scattering light intensity, M and N are constant, and the phase difference of 2 π/3 is differed between three tunnel output lights;
B. disappear DC component, and three road output intensity phase adductions average to obtain DC component, tri- tunnel output optical signal of Zai Yong DC component is subtracted, if DC component is in (1) formula
(3) formula is subtracted with (1) formula to obtain
C. phase to be measured is asked using antitrigonometric function;
Δ L indicates reference arm delay line length in interferometer, vBIndicate Brillouin shift, cnIndicate the light velocity in medium;
vB(t)=vB0(1+0.048×106ε) (6)
Find out that strain will lead to Brillouin shift and change by (5) (6) formula, changes, adopt so as to cause phase difference Phase demodulating is carried out with antitrigonometric function method, Brillouin shift variable quantity can be demodulated according to the variation of different moments phase, Obtain the vibration variation along sensor fibre.
Stimulated Brillouin scattering threshold value is lower than using pump power when spontaneous brillouin scattering.
The beneficial effects of the present invention are:
(1) pump power is lower than stimulated Brillouin scattering threshold value when surveying strain variation using spontaneous brillouin scattering, one Determine pump power needed for transmission same distance in SNR ranges to be lower than based on pump power needed for Rayleigh scattering sensing.
(2) phase demodulating is carried out using antitrigonometric function method, it is higher than the phase accuracy that differential multiplication cross method obtains.
Detailed description of the invention
Fig. 1 is antitrigonometric function method demodulation phase algorithm pattern.
Fig. 2 is to survey stress change principle figure based on spontaneous Brillouin back scattering.
Fig. 3 is the comparison diagram of the antitrigonometric function method that the present invention uses and differential multiplication cross method demodulation phase.
Specific embodiment
The invention proposes one kind to be based on phase-BOTDR Brillouin fiber optic distribution vibrating sensing measurement method, to realize The dynamic strain measurement of phase sensitive in distributing optical fiber sensing.Specific embodiment is as described below, includes distributed Feedback Laser source, Polarization Controller, pulse-modulator, erbium-doped fiber amplifier, optical circulator, single mode sensor fibre, optical fiber Bragg Grating, non-equilibrium Mach Zehnder interferometer, photodetector and data acquisition processing system, the distributed feedback laser source The continuous light issued is successively modulated into pulsed light through Polarization Controller, pulse-modulator, is put by erbium-doped fiber amplifier Greatly, amplified pulsed light enters single mode sensor fibre through optical circulator, and the backward Brillouin scattering light at vibration variation occurs Enter fiber bragg grating through optical circulator again, Brillouin scattering is interfered through non-equilibrium Mach Zehnder interferometer, defeated Tri- road light of Chu is handled after being received by a photoelectric detector by data acquisition processing system, is interfered using non-equilibrium Mach Zehnder Instrument structure converts the Brillouin shift variable quantity of back scattering to the variation of interference light output phase, according to different moments phase The variation of position demodulates Brillouin shift variable quantity, and then obtains the variation of the vibration along sensor fibre.
Using non-equilibrium Mach Zehnder interferometer structure, interference light is converted by the Brillouin shift variable quantity of back scattering The variation of phase is obtained Brillouin shift variation, realized using phase demodulating method using antitrigonometric function method demodulation phase Fiber-optic vibration measurement, the specific steps are as follows:
A. optical signal is acquired, three tunnel output optical signals are detected by photoelectric detector, backward Brillouin scattering light is by non- The three road light exported after the interference of balanced Mach Zehnder interferometer respectively indicate are as follows:
In above formula, I0For Brillouin scattering light intensity, M and N are constant, and the phase difference of 2 π/3 is differed between three tunnel output lights;
B. disappear DC component, and three road output intensity phase adductions average to obtain DC component, tri- tunnel output optical signal of Zai Yong DC component is subtracted, if DC component is in (1) formula
(3) formula is subtracted with (1) formula to obtain
C. phase to be measured is asked using antitrigonometric function;
Δ L indicates reference arm delay line length in interferometer, vBIndicate Brillouin shift, cnIndicate the light velocity in medium;
vB(t)=vB0(1+0.048×106ε) (6)
It can be seen that strain will lead to Brillouin shift and change by (5) (6) formula, as shown in Figure 1, 2.So as to cause phase Potential difference changes.Phase demodulating is carried out using antitrigonometric function method, as shown in Figure 3.It can according to the variation of different moments phase To demodulate Brillouin shift variable quantity, and then obtain the variation of the vibration along sensor fibre.

Claims (2)

1. one kind is based on phase-BOTDR Brillouin fiber optic distribution vibrating sensing measurement method, it is characterised in that: include point Cloth feedback laser source, Polarization Controller, pulse-modulator, erbium-doped fiber amplifier, optical circulator, single mode sensor fibre, light Fine Bragg grating, non-equilibrium Mach Zehnder interferometer, photodetector and data acquisition processing system, the distribution are anti- The continuous light that feedback laser source issues successively is modulated into pulsed light through Polarization Controller, pulse-modulator, passes through Erbium-doped fiber amplifier Device amplifies, and amplified pulsed light enters single mode sensor fibre through optical circulator, occurs in the backward cloth at vibration variation Deep pool scattering light enters fiber bragg grating through optical circulator again, and Brillouin scattering occurs through non-equilibrium Mach Zehnder interferometer Interference, three road light of output are handled after being received by a photoelectric detector by data acquisition processing system, and non-equilibrium Mach is utilized Zehnder interferometer structure converts the Brillouin shift variable quantity of back scattering to the variation of interference light output phase, according to not The variation of phase demodulates Brillouin shift variable quantity in the same time, and then obtains the variation of the vibration along sensor fibre.
2. according to claim 1 be based on phase-BOTDR Brillouin fiber optic distribution vibrating sensing measurement method, spy Sign is: utilizing non-equilibrium Mach Zehnder interferometer structure, converts interference light for the Brillouin shift variable quantity of back scattering The variation of phase is obtained Brillouin shift variation, realized using phase demodulating method using antitrigonometric function method demodulation phase Fiber-optic vibration measurement, the specific steps are as follows:
A. optical signal is acquired, three tunnel output optical signals are detected by photoelectric detector, backward Brillouin scattering light is by non-equilibrium The three road light exported after Mach Zehnder interferometer interference respectively indicate are as follows:
In above formula, I0For Brillouin scattering light intensity, M and N are constant, and the phase difference of 2 π/3 is differed between three tunnel output lights;
B. disappear DC component, and three road output intensity phase adductions average to obtain DC component, and tri- tunnel output optical signal of Zai Yong subtracts DC component, if DC component is in (1) formula
(3) formula is subtracted with (1) formula to obtain
C. phase to be measured is asked using antitrigonometric function;
Δ L indicates reference arm delay line length in interferometer, vBIndicate Brillouin shift, cnIndicate the light velocity in medium;
vB(t)=vB0(1+0.048×106ε) (6)
Find out that strain will lead to Brillouin shift and change by (5) (6) formula, changes so as to cause phase difference, using anti- Trigonometric function method carries out phase demodulating, can demodulate Brillouin shift variable quantity according to the variation of different moments phase, obtain Vibration variation along sensor fibre.
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Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111289222A (en) * 2020-01-21 2020-06-16 丽水正阳电力建设有限公司 An optical fiber breakpoint monitoring device based on phase sensitive optical time domain reflectometry
CN111458059A (en) * 2019-01-21 2020-07-28 中国科学院上海光学精密机械研究所 A continuous vehicle collision detection system and method thereof
CN113155165A (en) * 2021-05-14 2021-07-23 武汉理工大学 Interference type demodulation system and method for large-capacity fiber grating sensor network
CN114061638A (en) * 2021-10-26 2022-02-18 广东工业大学 Brillouin optical time domain reflectometer and phase demodulation method and device thereof
CN115290235A (en) * 2022-08-17 2022-11-04 广东工业大学 Method and device for phase demodulation of double-path quadrature signal in Brillouin optical time domain reflectometer
CN117968822A (en) * 2024-03-28 2024-05-03 深圳大学 A multi-point vibration positioning method based on forward distributed sensing and phase demodulation

Citations (21)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH11160200A (en) * 1997-10-02 1999-06-18 Furukawa Electric Co Ltd:The Distribution type sensor device nd distribution type sensing method
JP2000089177A (en) * 1998-09-10 2000-03-31 Oki Electric Ind Co Ltd Optical signal transmission device for optical communication system
CN1687811A (en) * 2005-04-29 2005-10-26 中国科学院上海光学精密机械研究所 Fiber Bragg Grating Wavelength Demodulator
CN1752836A (en) * 2005-09-27 2006-03-29 北京理工大学 A demodulation method of optical fiber interference signal
US20080019704A1 (en) * 2006-05-31 2008-01-24 Campillo Anthony L Interferometer-based chromatic dispersion monitor
CN101718563A (en) * 2009-12-09 2010-06-02 北京理工大学 Phase-shift white light interferometry method based on 3*3 optical fiber coupler
JP5021221B2 (en) * 2006-03-09 2012-09-05 ニューブレクス株式会社 Distributed optical fiber sensor
CN102809387A (en) * 2012-08-17 2012-12-05 东北大学 Novel BOTDR signal demodulating method
US20130071124A1 (en) * 2011-09-20 2013-03-21 Chongjin Xie Coherent Optical Receivers For Colorless Reception
CN103016851A (en) * 2012-12-06 2013-04-03 同济大学 Smart pipeline with optical fiber sensing function and manufacturing method for smart pipeline
CN103575220A (en) * 2013-10-31 2014-02-12 中国人民解放军国防科学技术大学 Miniaturization single-optical-grating interference measurement system and method based on optical fiber coupler
CN103604450A (en) * 2013-11-22 2014-02-26 哈尔滨理工大学 Seed injection BOTDR distributed optical fiber sensing system
CN104062031A (en) * 2014-07-16 2014-09-24 南昌航空大学 Long-distance and high-spatial-resolution sensing system based on cooperation between MZI sensing and Brillouin sensing
CN104567959A (en) * 2015-01-27 2015-04-29 中国人民解放军国防科学技术大学 Large-dynamic interference type optical fiber sensor based on two-channel unbalanced interferometer
CN104776871A (en) * 2015-01-30 2015-07-15 佛山科学技术学院 Fiber optic Brillouin distributed measurement optical path, device and method
CN105067017A (en) * 2015-06-02 2015-11-18 哈尔滨工程大学 Modified phase generated carrier (PGC) demodulation method
CN105222815A (en) * 2015-09-18 2016-01-06 南京派光信息技术有限公司 Based on the phase sensitive optical time domain reflectometer of 120 degree of difference interferometers
CN105865500A (en) * 2016-06-08 2016-08-17 北京理工大学 Phase shifting demodulation method of optical fiber laser interference type sensor
CN105910546A (en) * 2016-04-20 2016-08-31 北京信息科技大学 BOTDR system based on dual-channel Mach-Zehnder interferometer
CN105953724A (en) * 2016-04-20 2016-09-21 北京信息科技大学 Two-channel adjustable Mach-Zehnder interferometer
WO2018005539A1 (en) * 2016-06-27 2018-01-04 The Regents Of The University Of California Distributed dynamic strain fiber optics measurement by brillouin optical time-domain reflectometry

Patent Citations (21)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH11160200A (en) * 1997-10-02 1999-06-18 Furukawa Electric Co Ltd:The Distribution type sensor device nd distribution type sensing method
JP2000089177A (en) * 1998-09-10 2000-03-31 Oki Electric Ind Co Ltd Optical signal transmission device for optical communication system
CN1687811A (en) * 2005-04-29 2005-10-26 中国科学院上海光学精密机械研究所 Fiber Bragg Grating Wavelength Demodulator
CN1752836A (en) * 2005-09-27 2006-03-29 北京理工大学 A demodulation method of optical fiber interference signal
JP5021221B2 (en) * 2006-03-09 2012-09-05 ニューブレクス株式会社 Distributed optical fiber sensor
US20080019704A1 (en) * 2006-05-31 2008-01-24 Campillo Anthony L Interferometer-based chromatic dispersion monitor
CN101718563A (en) * 2009-12-09 2010-06-02 北京理工大学 Phase-shift white light interferometry method based on 3*3 optical fiber coupler
US20130071124A1 (en) * 2011-09-20 2013-03-21 Chongjin Xie Coherent Optical Receivers For Colorless Reception
CN102809387A (en) * 2012-08-17 2012-12-05 东北大学 Novel BOTDR signal demodulating method
CN103016851A (en) * 2012-12-06 2013-04-03 同济大学 Smart pipeline with optical fiber sensing function and manufacturing method for smart pipeline
CN103575220A (en) * 2013-10-31 2014-02-12 中国人民解放军国防科学技术大学 Miniaturization single-optical-grating interference measurement system and method based on optical fiber coupler
CN103604450A (en) * 2013-11-22 2014-02-26 哈尔滨理工大学 Seed injection BOTDR distributed optical fiber sensing system
CN104062031A (en) * 2014-07-16 2014-09-24 南昌航空大学 Long-distance and high-spatial-resolution sensing system based on cooperation between MZI sensing and Brillouin sensing
CN104567959A (en) * 2015-01-27 2015-04-29 中国人民解放军国防科学技术大学 Large-dynamic interference type optical fiber sensor based on two-channel unbalanced interferometer
CN104776871A (en) * 2015-01-30 2015-07-15 佛山科学技术学院 Fiber optic Brillouin distributed measurement optical path, device and method
CN105067017A (en) * 2015-06-02 2015-11-18 哈尔滨工程大学 Modified phase generated carrier (PGC) demodulation method
CN105222815A (en) * 2015-09-18 2016-01-06 南京派光信息技术有限公司 Based on the phase sensitive optical time domain reflectometer of 120 degree of difference interferometers
CN105910546A (en) * 2016-04-20 2016-08-31 北京信息科技大学 BOTDR system based on dual-channel Mach-Zehnder interferometer
CN105953724A (en) * 2016-04-20 2016-09-21 北京信息科技大学 Two-channel adjustable Mach-Zehnder interferometer
CN105865500A (en) * 2016-06-08 2016-08-17 北京理工大学 Phase shifting demodulation method of optical fiber laser interference type sensor
WO2018005539A1 (en) * 2016-06-27 2018-01-04 The Regents Of The University Of California Distributed dynamic strain fiber optics measurement by brillouin optical time-domain reflectometry

Non-Patent Citations (5)

* Cited by examiner, † Cited by third party
Title
M D TODD 等: ""A novel Bragg grating sensor interrogation system utilizing a scanning filter, a Mach-Zehnder interferometer and a coupler"", 《MEAS. SCI. TECHNOL》 *
M.D. TODD 等: ""Improved, operationally-passive interferometric demodulation method using 3x3 coupler"", 《ELECTRONKS LETTERS》 *
何玉钧 等: ""全光纤Mach-Zehnder 干涉仪及其在光纤自发布里渊散射测量中的应用"", 《光子学报》 *
朱晓非: ""基于相位检测的布里渊分布式光纤振动传感技术研究"", 《中国优秀硕士学位论文全文数据库》 *
毛欣 等: ""采用3 × 3 耦合器的分布反馈式光纤激光传感器解调技术"", 《发光学报》 *

Cited By (10)

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CN111458059A (en) * 2019-01-21 2020-07-28 中国科学院上海光学精密机械研究所 A continuous vehicle collision detection system and method thereof
CN111289222A (en) * 2020-01-21 2020-06-16 丽水正阳电力建设有限公司 An optical fiber breakpoint monitoring device based on phase sensitive optical time domain reflectometry
CN113155165A (en) * 2021-05-14 2021-07-23 武汉理工大学 Interference type demodulation system and method for large-capacity fiber grating sensor network
CN113155165B (en) * 2021-05-14 2022-07-05 武汉理工大学 Interference type demodulation system and method for large-capacity fiber grating sensor network
CN114061638A (en) * 2021-10-26 2022-02-18 广东工业大学 Brillouin optical time domain reflectometer and phase demodulation method and device thereof
CN114061638B (en) * 2021-10-26 2024-03-26 广东工业大学 Brillouin optical time domain reflectometer and phase demodulation method and device thereof
CN115290235A (en) * 2022-08-17 2022-11-04 广东工业大学 Method and device for phase demodulation of double-path quadrature signal in Brillouin optical time domain reflectometer
CN115290235B (en) * 2022-08-17 2024-07-23 广东工业大学 Phase demodulation method and device for dual-path orthogonal signals of Brillouin optical time domain reflectometer
CN117968822A (en) * 2024-03-28 2024-05-03 深圳大学 A multi-point vibration positioning method based on forward distributed sensing and phase demodulation
CN117968822B (en) * 2024-03-28 2024-06-21 深圳大学 A multi-point vibration positioning method based on forward distributed sensing and phase demodulation

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