CN109297425A - A kind of Brillouin optical time-domain reflectometer of physical random number modulation - Google Patents

A kind of Brillouin optical time-domain reflectometer of physical random number modulation Download PDF

Info

Publication number
CN109297425A
CN109297425A CN201810968261.0A CN201810968261A CN109297425A CN 109297425 A CN109297425 A CN 109297425A CN 201810968261 A CN201810968261 A CN 201810968261A CN 109297425 A CN109297425 A CN 109297425A
Authority
CN
China
Prior art keywords
fiber coupler
brillouin
optical
fiber
random number
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201810968261.0A
Other languages
Chinese (zh)
Other versions
CN109297425B (en
Inventor
王宇
白清
谷行
靳宝全
王云才
王东
刘昕
田振东
郭凌龙
高妍
张建国
张红娟
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Taiyuan University of Technology
Original Assignee
Taiyuan University of Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Taiyuan University of Technology filed Critical Taiyuan University of Technology
Priority to CN201810968261.0A priority Critical patent/CN109297425B/en
Publication of CN109297425A publication Critical patent/CN109297425A/en
Application granted granted Critical
Publication of CN109297425B publication Critical patent/CN109297425B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/16Measuring arrangements characterised by the use of optical techniques for measuring the deformation in a solid, e.g. optical strain gauge
    • G01B11/18Measuring arrangements characterised by the use of optical techniques for measuring the deformation in a solid, e.g. optical strain gauge using photoelastic elements

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optical Communication System (AREA)

Abstract

The invention belongs to Distributed Optical Fiber Sensing Techniques fields, for the spatial resolution of Brillouin optical time-domain reflectometer in the prior art, the compromise problem of signal-to-noise ratio and measurement accuracy, propose a kind of Brillouin optical time-domain reflectometer of physical random number modulation, including the first DFB laser emitting module, 2nd DFB laser emitting module, first fiber coupler, pulse image intensifer, second fiber coupler, Polarization Controller, gain switch modulator, module occurs for physical random number, DWDM dense wavelength division multiplexing device, sensor fibre, optical fiber circulator, continuous image intensifer, optical filter, third fiber coupler, scrambler, photodetector, frequency mixer, microwave tunable frequency source, electric amplifier, electrical filter, A/D conversion module and host computer.The present invention can be under the premise of guaranteeing spatial resolution, strain size and the position of real-time high-precision monitored along sensor fibre.

Description

A kind of Brillouin optical time-domain reflectometer of physical random number modulation
Technical field
The present invention relates to Brillouin optical time-domain reflectometers, belong to Distributed Optical Fiber Sensing Techniques field, more specifically, this Invention is related to a kind of Brillouin optical time-domain reflectometer of physical random number modulation.
Background technique
In recent years, distributing optical fiber sensing detection technique is grown rapidly, compared with quasi-distributed optical fiber sensing, point Cloth optical fiber sensing technology will be sensed and is combined into one with transmission, can measure the environmental change letter of all positions along whole optical fiber Breath, has the characteristics that electromagnetism interference, corrosion-resistant, long distance transmission, structure is simple, range of dynamic measurement is big, therefore answer extensively It is a wide range of for heavy construction, highway, dam, the monitoring structural health conditions of bridge and underground pipe network, oil-gas pipeline etc., long away from Safety monitoring under.Wherein, Brillouin optical time-domain reflectometer is suitable for the strain detecting of long range, and principle is according to optical fiber The frequency displacement linear relationship corresponding with strain that middle spontaneous brillouin scattering signal generates detects strain information, and in conjunction with OTDR (optical time domain reflection) technology realizes the positioning to strain point.Currently based on the distributed sensing skill of Brillouin light Time Domain Reflectometry In art, BOTDR (Brillouin light time domain reflection technology) and BOTDA (Brillouin light frequency-domain analysis technology) are the skills of two kinds of mainstreams Art.BOTDA system needs the light source of both-end to inject, and cannot detect to breakpoint along optical fiber, use occasion is limited to. BOTDR system carries out sensing measurement by way of single-ended injection, it can be achieved that positioning to breakpoint, is that everybody current use is most wide A kind of general technology, but its weak output signal, signal-to-noise ratio is smaller and smaller, to the more demanding of system signal demodulation.In order to solve Under conditions of time of measuring and spatial resolution are constant, the signal-to-noise ratio problem of lifting system, some is used in currently existing scheme Cumulative mean Time Method, some uses increase the method for pulse width, the coding modes such as use Golay also, but these sides Method all has the defect of its own: the time of measuring of system can be made to greatly prolong using cumulative mean Time Method, influence system Real-time;If increasing pulse width, spatial resolution will certainly be reduced, influences system for the accuracy of small event;If adopting With the coding modes such as Golay be easy so that four groups of coded pulses decoding when intersymbol interference occurs, influence the demodulation accuracy of system. Existing method can not all solve the problems, such as the compromise of System spatial resolution, signal-to-noise ratio and measurement accuracy, it is, therefore, desirable to provide one The high Brillouin optical time-domain reflectometer of kind signal-to-noise ratio.
Summary of the invention
The present invention overcomes the shortcomings of Brillouin's time-domain reflectomer in the prior art, technical problem to be solved are as follows: provides A kind of Brillouin optical time-domain reflectometer of physical random number modulation, by physical random number generator module, primary one group of injection Real random code obtains additional coding gain, improves system signal noise ratio, the crosstalk between there is not code word, and spatial resolution does not change Under the premise of change, whole power informations of Brillouin scattering are effectively restored in real time.
In order to solve the above-mentioned technical problem, the technical solution adopted by the present invention are as follows: in a kind of cloth of physical random number modulation Deep optical time domain reflectometer, including the first DFB laser emitting module, the 2nd DFB laser emitting module, the first fiber coupler, arteries and veins It is close to wash amplifier, the second fiber coupler, Polarization Controller, gain switch modulator, physical random number generation module, DWDM off Collection type wavelength division multiplexer, optical fiber circulator, continuous image intensifer, optical filter, third fiber coupler, is disturbed partially at sensor fibre Device, photodetector, frequency mixer, microwave tunable frequency source, electric amplifier, electrical filter, A/D conversion module and host computer;Institute The continuous optical signal for stating the sending of the first DFB laser emitting module is output to the input terminal of the second fiber coupler, through the second optical fiber Coupler is divided into reference light and detection light two parts, wherein detection light is exported from the first output end of the second fiber coupler, warp After Polarization Controller, gain switch modulator, it is output to the first input end of the first fiber coupler;The 2nd DFB laser Transmitting module issues the second input terminal that continuous optical signal is output to the first fiber coupler;First fiber coupler it is defeated Outlet is connect after pulsed light amplifier, DWDM dense wavelength division multiplexing device with the first port of optical fiber circulator, fiber annular The second port of device is connect with sensor fibre, and the third port of optical fiber circulator is connect with the input terminal of continuous image intensifer, right Faint backward Brillouin scattering signal carries out power amplification, and the output end of the continuous image intensifer is after optical filter with the The first input end of three fiber couplers connects;The reference light of the second output terminal output of second fiber coupler is disturbed partially It is connect after device with the second input terminal of third fiber coupler;The output signal of the third fiber coupler is by photodetector Detection, the output signal of the photodetector is mixed with the microwave signal that microwave tunable frequency source emits through frequency mixer, electricity is put Host computer is output to after big device, electrical filter, A/D conversion module;Module occurs for the physical random number for generating two groups of phases Same real random code modulates continuous optical signal wherein one group of real random code is sent to the control terminal of gain switch modulator At sequential coding pulsed optical signals, another group of real random code is sent to host computer, and the host computer is used for according to described truly random Code is decoded operation to brillouin scattering signal, demodulates Brillouin shift distribution.
First fiber coupler, the second fiber coupler and third fiber coupler are 1 × 2 fiber coupling The splitting ratio of device, first fiber coupler and third fiber coupler is 50:50, the light splitting of second fiber coupler Than for 80:20.
The continuous optical signal that first DFB laser emitting module is used to issue central wavelength as 1550.12nm, described second DFB laser emitting module is used to issue the continuous optical signal that central wavelength is 1560.12nm.
Related operation unit and cumulative mean processing unit are provided in the host computer, the host computer carries out related fortune Calculation and cumulative mean operation demodulate Brillouin shift distribution method particularly includes:
Related operation unit carries out related operation with first brillouin scattering signal to first part's coded strings of real random code Processing, obtains the noisy Brillouin shift distribution curve of the first band;Second part of the related operation unit to real random code Coded strings and Article 2 brillouin scattering signal carry out related computing, obtain the noisy Brillouin shift of second strip point Cloth curve;……;Related operation unit carries out phase with nth brillouin scattering signal to the n-th code segment string of real random code Calculation process is closed, the noisy Brillouin shift distribution curve of nth band is obtained, the Brillouin until completing all different frequencies Frequency displacement distribution curve;Related operation unit is connect with cumulative mean processing unit, the noisy brillouin frequency of n band that will be obtained It moves distribution curve and is sent to the cumulative mean processing unit;Obtained n item is had noise by the cumulative mean processing unit Brillouin shift distribution curve carry out cumulative mean processing, obtain Brillouin scattering curve, the n is indicated in real random code The quantity of coded strings.
Working principle of the present invention is as follows: physical random number occurs module 8 and is simultaneously emitted by two groups of identical real random codes, In in one group of feeding gain switch modulator, be sequential coding pulsed light by detection light modulation, squeeze into optical fiber, what is obtained is backward scattered It penetrates signal and carries out beat frequency processing in photodetector 16 with by the reference signal of scrambler 15, obtain Brillouin shift letter Breath;The different frequency signals that microwave tunable frequency source 18 issues successively carry out difference frequency processing with Brillouin shift by frequency mixer, Performed a scan by the electrical filter 20 of fixed-bandwidth, obtain brillouin scattering signal, after A/D is converted with physical accidental Another group of real random code that the sending of module 8 occurs is counted in host computer by way of related operation, cumulative mean, lifting system Signal-to-noise ratio.Sequential coding pulse is the superposition of pulse, and System spatial resolution depends on the pulsewidth of pulse, with pulse String itself is unrelated, therefore train pulse coding only improves coding gain, does not change scattered signal and changes with time, to realize The high-precision measurement under spatial resolution permanence condition.
The Brillouin optical time-domain reflectometer and decoding scheme of a kind of physical random number modulation provided by the invention, and it is existing Distributive fiber optic strain detection is compared, high reliablity, at low cost, achievable high-resolution and high-precision strain detecting, excellent Point is as follows with good effect major embodiment:
One, physical random number itself has good correlation properties, by the available volume of sequential coding impulses injection sensor fibre Outer coding gain improves system signal noise ratio.Meanwhile physical random number and coding brillouin scattering signal are utilized in decoding process Multiple related average calculating operation can further decrease system noise, improve anti-interference and measurement accuracy.
Two, compared with traditional electro-optical pulse modulation scheme, can be stablized using gain switch modulator and higher Direct impulse extinction ratio can save bias control device necessary to traditional Electro-optical Modulation scheme, to save the cost and reduce System complexity;Meanwhile can avoid electrooptic modulator insertion loss, guarantee it is higher enter fine peak power.
Three, using the second narrow linewidth DFB laser emitting module of 1560.12nm wavelength, it is possible to reduce pulse image intensifer The influence that amplification unevenly generates sequential coding pulsed light.
Detailed description of the invention
Fig. 1 is that a kind of structure of the Brillouin optical time-domain reflectometer of physical random number modulation provided in an embodiment of the present invention is shown It is intended to;
Fig. 2 is the schematic diagram of Brillouin optical time-domain reflectometer decoding scheme in the embodiment of the present invention.
In figure: 1 is the first narrow linewidth DFB laser emitting module, and 2 be the second narrow linewidth DFB laser emitting module, and 3 be the One fiber coupler, 4 be pulse image intensifer, and 5 be the second fiber coupler, and 6 be Polarization Controller, and 7 modulate for gain switch Device, 8 occur module for physical random number, and 9 be DWDM dense wavelength division multiplexing device, and 10 be sensor fibre, and 11 be optical fiber circulator, 12 be continuous image intensifer, and 13 be optical filter, and 14 be third fiber coupler, and 15 be scrambler, and 16 be photodetector, 17 It is microwave tunable frequency source for frequency mixer, 18,19 be electric amplifier, and 20 be electrical filter, and 21 be A/D conversion module, and 22 be upper Position machine, 23 be real random code, and 24 be brillouin scattering signal, and 25 be related operation unit, and 26 be cumulative mean processing unit, 27 For Brillouin scattering curve.
Specific embodiment
It in order to make the object, technical scheme and advantages of the embodiment of the invention clearer, below will be in the embodiment of the present invention Technical solution be clearly and completely described, it is clear that described embodiment is a part of the embodiments of the present invention, without It is whole embodiments;Based on the embodiments of the present invention, those of ordinary skill in the art are not before making creative work Every other embodiment obtained is put, shall fall within the protection scope of the present invention.
Embodiment one
As shown in Figure 1, present embodiments providing a kind of Brillouin optical time-domain reflectometer of physical random number modulation, including first DFB laser emitting module 1, the 2nd DFB laser emitting module 2, the first fiber coupler 3, pulse image intensifer 4, the second optical fiber Module 8, DWDM dense wavelength division multiplexing device occur for coupler 5, Polarization Controller 6, gain switch modulator 7, physical random number 9, sensor fibre 10, optical fiber circulator 11, continuous image intensifer 12, optical filter 13, third fiber coupler 14, scrambler 15, photodetector 16, frequency mixer 17, microwave tunable frequency source 18, electric amplifier 19, electrical filter 20, A/D conversion module 21 With host computer 22.
Wherein, the first DFB laser emitting module 1 issues the continuous light letter of narrow linewidth that central wavelength is 1550.12nm Number, which is output to the input terminal A of the second fiber coupler 5, and the reference for 20% is divided through the second fiber coupler 5 Light and 80% detection light two parts, wherein detection light from the first output end B of the second fiber coupler 5 export, through Polarization Control It is inputted after device 6 from the input port D of gain switch modulator 7, is output to the first light from the output port E of gain switch modulator The first input end of fine coupler 3;The 2nd DFB laser emitting module 2 issues the continuous light that central wavelength is 1560.12nm Signal, the continuous optical signal are output to the second input terminal of the first fiber coupler 3.Polarization Controller 6 is for adjusting continuous spy The polarization state for surveying light makes light reach optimal laser propagation effect;Mould occurs for the control terminal F and physical random number of gain switch modulator 7 First output end of block 8 connects, and module 8 occurs for the physical random number for generating two groups of identical real random codes, wherein one Group real random code is sent to the control terminal F of gain switch modulator 7, and continuous optical signal is made to be modulated into sequential coding pulsed light letter Number, wherein the length of random code is longer, and the gain coefficient for controlling gain switch modulator is bigger, and another group of real random code is sent To the input port M of host computer 22.
Wherein, the output end of first fiber coupler 3 is connected to the input terminal of pulse image intensifer 4, compiles to sequence Code pulse carry out power amplification, with this obtain it is higher enter fine peak power, while the 2nd DFB laser emitting module 2 output The continuous light of 1560.12nm wavelength keeps the concentration of erbium ion for consuming the more erbium ion in 4 front end of pulse image intensifer It is constant, to reduce the influence that the amplification of pulse image intensifer unevenly generates sequential coding pulsed light;The pulse light amplification The output end of device 4 is connected to the input terminal of DWDM dense wavelength division multiplexing device 9, filters out spontaneous radiation caused by pulse image intensifer The continuous light of noise and 1560.12nm wavelength makes the sequential coding pulsed light of 1550.12nm carry out onwards transmission;The DWDM The output end of dense wavelength division multiplexing device 9 is connected to the first port G of optical fiber circulator 11, and the second of the optical fiber circulator 11 Port H is connected to the sensor fibre 10 of common G652 single mode, and sequence pulse code enters fiber annular through first port G at this time Device 11 is exported from the second port H of optical fiber circulator 11 into after sensor fibre 10, generates backward Brillouin scattering signal, from The faint backward Brillouin scattering signal returned in sensor fibre 10 enters optical fiber circulator 11 through second port H, and from institute The third port I output of optical fiber circulator 11 is stated, the third port I of the optical fiber circulator 11 is defeated with continuous image intensifer 12 Enter end connection, continuous image intensifer 12 is output to optical filter after carrying out power amplification to faint backward Brillouin scattering signal 13 input terminal, optical filter 13 export brillouin scattering signal after filtering out the noise of amplifier itself, the noise in environment To the first input end of the third fiber coupler 14.
In addition, the reference light that exports of the second output terminal C of second fiber coupler 5 after scrambler 15 with third light Second input terminal of fine coupler 14 connects, and scrambler 15 can guarantee that reference light has good polarization state, third optical fiber The splitting ratio of the input terminal of coupler 14 is 50:50;The output signal of the third fiber coupler 14 is by photodetector 16 Reference light and detection light are carried out beat frequency, obtain Brillouin shift information with this by detection, photodetector 16;The photodetection The output end of device 16 is connected to the input terminal J of frequency mixer 17, carries out down conversion process;The output end of the microwave tunable frequency source 18 It is connected to the input terminal K of frequency mixer 17, changes the frequency size of Brillouin shift with this;The output end L of the frequency mixer 17 connects It is connected to the input terminal of electric amplifier 19, this faint continuous signal is amplified;This signal, which enters in electrical filter 20, to be passed through The mode of frequency scanning obtains system brillouin scattering signal 24.The output port of electrical filter 20 passes through A/D conversion module 21 The input port N for being output to host computer 22, the host computer is used for according to the real random code inputted from input port M to from defeated The brillouin scattering signal of inbound port N input is decoded operation, demodulates Brillouin scattering curve.
In the present embodiment, first fiber coupler 3, the second fiber coupler 5 and third fiber coupler 14 are The splitting ratio of 1 × 2 fiber coupler, first fiber coupler 3 and third fiber coupler 14 is 50:50, described the The splitting ratio of two fiber couplers 5 is 80:20.
Embodiment two
The structure and first embodiment phase of a kind of Brillouin optical time-domain reflectometer of physical random number modulation provided in this embodiment It together, the difference is that, when host computer 22 is decoded operation, is transported by related operation and cumulative mean in the present embodiment It calculates, Brillouin shift distribution is demodulated, as shown in Fig. 2, being provided with related operation unit 25 and cumulative mean in host computer 22 Processing unit 26, related operation unit 25 are connect with cumulative mean processing unit 26, the detailed process being decoded are as follows:
The first input port M that the real random code 23 that module 8 issues inputs host computer 22, cloth occur for S1, the physical random number In deep scattered signal 24 the second input port N of host computer 22 is inputted after the A/D conversion module 21 is converted to digital signal.
S2, related operation unit 25 carry out related operation, method particularly includes: related operation unit 25 is to real random code 23 First part's coded strings carry out related computing with first brillouin scattering signal 24, obtain the noisy cloth of the first band In deep frequency displacement distribution curve;Second part coded strings and Article 2 Brillouin scattering of the related operation unit 25 to real random code 23 Signal carries out related computing, obtains the noisy Brillouin shift distribution curve of second strip;……;Related operation unit The the n-th code segment string and nth brillouin scattering signal of 25 pairs of real random codes 23 carry out related computing, obtain nth Brillouin shift distribution curve with noisy Brillouin shift distribution curve, until completing all different frequencies;The n table Show the quantity of the coded strings in real random code 23.
S3, cumulative mean processing unit 26 carry out cumulative mean processing, method particularly includes: related operation unit 25 will obtain The noisy Brillouin shift distribution curve of n band be sent to the cumulative mean processing unit 26;At the cumulative mean The noisy Brillouin shift distribution curve of this n band be averaging processing again after adding up by reason unit 26, obtains in cloth Deep scattering curve 27.
The invention proposes a kind of Brillouin optical time-domain reflectometers of physical random number modulation, due to physical random number itself With good correlation properties, by the available additional coding gain of sequential coding impulses injection sensor fibre, therefore this hair It is bright to improve system signal noise ratio;Meanwhile the present invention utilizes physical random number and coding brillouin scattering signal in decoding process Multiple related average calculating operation can further decrease system noise, improve anti-interference and measurement accuracy, solve system space Under the premise of resolution ratio is constant, signal-to-noise ratio promotes the problem of improving measurement accuracy, in addition, being modulated in the present invention using gain switch Device can save bias control device necessary to traditional Electro-optical Modulation scheme, to save the cost and reduce system complexity;Together When, can avoid electrooptic modulator insertion loss, guarantee it is higher enter fine peak power.The present invention can guarantee spatial discrimination Strain size and position under the premise of rate, along the monitoring sensor fibre of real-time high-precision.
Finally, it should be noted that the above embodiments are only used to illustrate the technical solution of the present invention., rather than its limitations;To the greatest extent Pipe present invention has been described in detail with reference to the aforementioned embodiments, those skilled in the art should understand that: its according to So be possible to modify the technical solutions described in the foregoing embodiments, or to some or all of the technical features into Row equivalent replacement;And these are modified or replaceed, various embodiments of the present invention technology that it does not separate the essence of the corresponding technical solution The range of scheme.

Claims (4)

1. a kind of Brillouin optical time-domain reflectometer of physical random number modulation, which is characterized in that including the first DFB Laser emission mould Block (1), the 2nd DFB laser emitting module (2), the first fiber coupler (3), pulse image intensifer (4), the second fiber coupler (5), module (8), DWDM dense wavelength division multiplexing occur for Polarization Controller (6), gain switch modulator (7), physical random number Device (9), sensor fibre (10), optical fiber circulator (11), continuous image intensifer (12), optical filter (13), third fiber coupling Device (14), scrambler (15), photodetector (16), frequency mixer (17), microwave tunable frequency source (18), electric amplifier (19), Electrical filter (20), A/D conversion module (21) and host computer (22);
The continuous optical signal that the first DFB laser emitting module (1) issues is output to the input of the second fiber coupler (5) End is divided into reference light and detection light two parts through the second fiber coupler (5), wherein detecting light from the second fiber coupler (5) The first output end output, after Polarization Controller (6), gain switch modulator (7), be output to the first fiber coupler (3) First input end;The 2nd DFB laser emitting module (2) issues continuous optical signal and is output to the first fiber coupler (3) The second input terminal;
The output end of first fiber coupler (3) is after pulsed light amplifier (4), DWDM dense wavelength division multiplexing device (9) It is connect with the first port of optical fiber circulator (11), the second port of optical fiber circulator (11) is connect with sensor fibre (10), light The third port of fine circulator (11) is connect with the input terminal of continuous image intensifer (12), is believed faint backward Brillouin scattering Number carry out power amplification, the output end of the continuous image intensifer (12) after optical filter (13) with third fiber coupler (14) first input end connection;
Second fiber coupler (5) second output terminal output reference light after scrambler (15) with third fiber coupling Second input terminal of device (14) connects;The output signal of the third fiber coupler (14) is detected by photodetector (16), The output signal of the photodetector (16) and the microwave signal of microwave tunable frequency source (18) transmitting are mixed through frequency mixer (17) Frequently, host computer (22) are output to after electric amplifier (19), electrical filter (20), A/D conversion module (21);
Module (8) occur for the physical random number for generating two groups of identical real random codes, wherein one group of real random code is sent To the control terminal of gain switch modulator (7), continuous optical signal is made to be modulated into sequential coding pulsed optical signals, another group very with Machine code is sent to host computer (22), and the host computer is used to be decoded fortune to brillouin scattering signal according to the real random code It calculates, demodulates Brillouin shift distribution.
2. a kind of Brillouin optical time-domain reflectometer of physical random number modulation according to claim 1, which is characterized in that institute State the fiber coupling that the first fiber coupler (3), the second fiber coupler (5) and third fiber coupler (14) are 1 × 2 The splitting ratio of device, first fiber coupler (3) and third fiber coupler (14) is 50:50, second fiber coupling The splitting ratio of device (5) is 80:20.
3. a kind of Brillouin optical time-domain reflectometer of physical random number modulation according to claim 1, which is characterized in that the One DFB laser emitting module (1) is used to issue the continuous optical signal that central wavelength is 1550.12nm, the 2nd DFB laser hair Module (2) are penetrated for issuing the continuous optical signal that central wavelength is 1560.12nm.
4. a kind of Brillouin optical time-domain reflectometer of physical random number modulation according to claim 1, which is characterized in that institute It states in host computer (22) and is provided with related operation unit (25) and cumulative mean processing unit (26);The host computer (22) carries out Related operation and cumulative mean operation demodulate Brillouin shift distribution method particularly includes:
First part coded strings and first brillouin scattering signal (24) of the related operation unit (25) to real random code (23) Related computing is carried out, the noisy Brillouin shift distribution curve of the first band is obtained;Related operation unit (25) is to true The second part coded strings and Article 2 brillouin scattering signal of random code (23) carry out related computing, obtain second strip Noisy Brillouin shift distribution curve;……;N-th code segment string of the related operation unit (25) to real random code (23) Related computing is carried out with nth brillouin scattering signal, obtains the noisy Brillouin shift distribution curve of nth band, Brillouin shift distribution curve until completing all different frequencies;Related operation unit (25) and cumulative mean processing unit (26) it connects, the noisy Brillouin shift distribution curve of obtained n band is sent to the cumulative mean processing unit (26);The cumulative mean processing unit (26) adds up the noisy Brillouin shift distribution curve of obtained n band Average treatment obtains Brillouin scattering curve (27), and the n indicates the quantity of the coded strings in real random code (23).
CN201810968261.0A 2018-08-23 2018-08-23 Brillouin optical time domain reflectometer modulated by physical random number Active CN109297425B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201810968261.0A CN109297425B (en) 2018-08-23 2018-08-23 Brillouin optical time domain reflectometer modulated by physical random number

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201810968261.0A CN109297425B (en) 2018-08-23 2018-08-23 Brillouin optical time domain reflectometer modulated by physical random number

Publications (2)

Publication Number Publication Date
CN109297425A true CN109297425A (en) 2019-02-01
CN109297425B CN109297425B (en) 2020-04-03

Family

ID=65165593

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201810968261.0A Active CN109297425B (en) 2018-08-23 2018-08-23 Brillouin optical time domain reflectometer modulated by physical random number

Country Status (1)

Country Link
CN (1) CN109297425B (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110375800A (en) * 2019-06-03 2019-10-25 太原理工大学 A kind of sensing device and method based on super continuous spectrums Brillouin light time domain analyzer
CN110632764A (en) * 2019-10-31 2019-12-31 太原理工大学 Chaotic light generating device based on TOAD ring
CN110632762A (en) * 2019-10-31 2019-12-31 太原理工大学 Device for generating chaotic light based on feedback interference principle
CN110632763A (en) * 2019-10-31 2019-12-31 太原理工大学 Method for generating chaotic light based on feedback interference principle
CN110795065A (en) * 2019-10-31 2020-02-14 太原理工大学 TOAD-based all-optical random number generation device
CN110806852A (en) * 2019-10-31 2020-02-18 太原理工大学 All-optical true random number generator based on feedback interference principle
CN111157026A (en) * 2020-02-12 2020-05-15 太原理工大学 Distributed optical fiber sensing detection device and method for railway rockfall protection net
CN112414584A (en) * 2020-10-19 2021-02-26 太原理工大学 Brillouin optical time domain analysis device and method based on pi-pulse Gray code coding

Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02186236A (en) * 1989-01-12 1990-07-20 Nippon Telegr & Teleph Corp <Ntt> Branch light beam path characteristic evaluation system
JPH0933389A (en) * 1995-07-24 1997-02-07 Advantest Corp Rear brillouin scattering light otdr device, measuring method therefor, and optical communication line system using this device
CN103674110A (en) * 2013-11-26 2014-03-26 北京航天时代光电科技有限公司 Distributed optical fiber temperature strain sensor based on Brillouin optical amplification detection
CN203672517U (en) * 2013-12-18 2014-06-25 中国能源建设集团广东省电力设计研究院 Brillouin scattering based distributed measurement system
CN103954311A (en) * 2014-03-11 2014-07-30 中国科学院上海光学精密机械研究所 Phase-sensitive optical time domain reflectometer based on Brillouin amplification
CN104111086A (en) * 2014-08-12 2014-10-22 盐城工学院 Low-Brillouin scattering threshold sensing fiber-based optical time domain reflectometer device and method
CN104266752A (en) * 2014-09-23 2015-01-07 李卫 Optical fiber backscattering measurement method and device based on spread spectrum technology
CN106441447A (en) * 2016-11-15 2017-02-22 太原理工大学 Chaos Brillouin dynamic grating based distributed optical fiber sensing system
CN107543567A (en) * 2017-08-11 2018-01-05 太原理工大学 BOCDA distribution type optical fiber sensing equipments and method based on the modulation of physical accidental code
CN107607135A (en) * 2017-09-19 2018-01-19 太原理工大学 A kind of chaos Brillouin light time domain/coherent field convergence analysis device and method
CN108180853A (en) * 2017-12-22 2018-06-19 太原理工大学 A kind of Brillouin light Time Domain Reflectometry strain-Sensing device based on chaotic modulation

Patent Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02186236A (en) * 1989-01-12 1990-07-20 Nippon Telegr & Teleph Corp <Ntt> Branch light beam path characteristic evaluation system
JPH0933389A (en) * 1995-07-24 1997-02-07 Advantest Corp Rear brillouin scattering light otdr device, measuring method therefor, and optical communication line system using this device
CN103674110A (en) * 2013-11-26 2014-03-26 北京航天时代光电科技有限公司 Distributed optical fiber temperature strain sensor based on Brillouin optical amplification detection
CN203672517U (en) * 2013-12-18 2014-06-25 中国能源建设集团广东省电力设计研究院 Brillouin scattering based distributed measurement system
CN103954311A (en) * 2014-03-11 2014-07-30 中国科学院上海光学精密机械研究所 Phase-sensitive optical time domain reflectometer based on Brillouin amplification
CN104111086A (en) * 2014-08-12 2014-10-22 盐城工学院 Low-Brillouin scattering threshold sensing fiber-based optical time domain reflectometer device and method
CN104266752A (en) * 2014-09-23 2015-01-07 李卫 Optical fiber backscattering measurement method and device based on spread spectrum technology
CN106441447A (en) * 2016-11-15 2017-02-22 太原理工大学 Chaos Brillouin dynamic grating based distributed optical fiber sensing system
CN107543567A (en) * 2017-08-11 2018-01-05 太原理工大学 BOCDA distribution type optical fiber sensing equipments and method based on the modulation of physical accidental code
CN107607135A (en) * 2017-09-19 2018-01-19 太原理工大学 A kind of chaos Brillouin light time domain/coherent field convergence analysis device and method
CN108180853A (en) * 2017-12-22 2018-06-19 太原理工大学 A kind of Brillouin light Time Domain Reflectometry strain-Sensing device based on chaotic modulation

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
T. SYMUL等: "Real time demonstration of high bitrate quantum random number generation with coherent laser light", 《APPLIED PHYSICS LETTERS》 *
刘瑞霞等: "一种利用布里渊增益谱边带解调提高布里渊光时域反射系统测温精度的方法", 《物理学报》 *
毛燕婷等: "脉冲编码光时域反射计技术", 《激光杂志》 *

Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110375800A (en) * 2019-06-03 2019-10-25 太原理工大学 A kind of sensing device and method based on super continuous spectrums Brillouin light time domain analyzer
CN110375800B (en) * 2019-06-03 2021-03-02 太原理工大学 Sensing device and method based on super-continuum spectrum Brillouin optical time domain analyzer
CN110632764A (en) * 2019-10-31 2019-12-31 太原理工大学 Chaotic light generating device based on TOAD ring
CN110632762A (en) * 2019-10-31 2019-12-31 太原理工大学 Device for generating chaotic light based on feedback interference principle
CN110632763A (en) * 2019-10-31 2019-12-31 太原理工大学 Method for generating chaotic light based on feedback interference principle
CN110795065A (en) * 2019-10-31 2020-02-14 太原理工大学 TOAD-based all-optical random number generation device
CN110806852A (en) * 2019-10-31 2020-02-18 太原理工大学 All-optical true random number generator based on feedback interference principle
CN110806852B (en) * 2019-10-31 2020-05-26 太原理工大学 All-optical true random number generator based on feedback interference principle
CN110632764B (en) * 2019-10-31 2021-05-25 太原理工大学 Chaotic light generating device based on TOAD ring
CN111157026A (en) * 2020-02-12 2020-05-15 太原理工大学 Distributed optical fiber sensing detection device and method for railway rockfall protection net
CN111157026B (en) * 2020-02-12 2021-07-02 太原理工大学 Distributed optical fiber sensing detection device and method for railway rockfall protection net
CN112414584A (en) * 2020-10-19 2021-02-26 太原理工大学 Brillouin optical time domain analysis device and method based on pi-pulse Gray code coding

Also Published As

Publication number Publication date
CN109297425B (en) 2020-04-03

Similar Documents

Publication Publication Date Title
CN109297425A (en) A kind of Brillouin optical time-domain reflectometer of physical random number modulation
CN107917738B (en) Distributed optical fiber sensing system capable of simultaneously measuring temperature, strain and vibration
CN107607135B (en) A kind of chaos Brillouin light time domain/coherent field convergence analysis device and method
CN101764646B (en) Wavelength-encoding optical time domain reflection test device and measurement method thereof
CN103152097B (en) A kind of adopt Random Laser to amplify polarization and phase sensitive optical time domain reflectometer
CN102589592B (en) Multi-wavelength light source-based Brillouin optical time domain reflectometer
CN102759371B (en) COTDR (coherent detection based optical time-domain reflectometry) fused long-distance coherent detection brilouin optical time-domain analyzer
CN102506904B (en) Spontaneous Brillouin scattering optical time domain reflectometer based on superconductive nanowire single-proton detector
CN106768277B (en) A kind of demodulation method of distributed optical fiber vibration sensing device
CN105806465B (en) A kind of novel Φ-OTDR detection device and its detection method based on fixation reflex point
CN103048070B (en) Stress monitoring method of distributed optical fiber system
CN110243493B (en) Brillouin optical time domain reflectometer device and method based on super-continuum spectrum
CN105067143B (en) A kind of homodyne Brillouin optical time-domain reflectometer based on Raman amplifiction
CN110375800B (en) Sensing device and method based on super-continuum spectrum Brillouin optical time domain analyzer
CN103644962A (en) Ultra long distance distributed optical fiber vibration sensing device
CN104792343A (en) Single-ended structure dynamic measuring Brillouin optical fiber sensing system and sensing method
CN110501062B (en) Distributed optical fiber sound sensing and positioning system
CN103076112B (en) The parameter measuring apparatus of single-side belt distributed optical fiber sensing system
CN203310428U (en) Distributed Brillouin optical fiber sensing system based on coherent detection
CN108801305B (en) Method and device of Brillouin optical time domain reflectometer based on step pulse self-amplification
US20230314188A1 (en) Self-heterodyne phi-otdr system with free multi-spatial resolution
CN111721338A (en) Brillouin optical time domain analysis system for alternately modulating high frequency and low frequency of pump light
CN103323041A (en) Distributed Brillouin optical fiber sensing system based on coherent detection
CN104111086A (en) Low-Brillouin scattering threshold sensing fiber-based optical time domain reflectometer device and method
CN106610303B (en) A kind of BOTDR method for sensing and system based on FFT and coding

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant