CN108593089A - A kind of vibration of optical sensor and inducing method based on birefringence resonance effect - Google Patents

A kind of vibration of optical sensor and inducing method based on birefringence resonance effect Download PDF

Info

Publication number
CN108593089A
CN108593089A CN201810410240.7A CN201810410240A CN108593089A CN 108593089 A CN108593089 A CN 108593089A CN 201810410240 A CN201810410240 A CN 201810410240A CN 108593089 A CN108593089 A CN 108593089A
Authority
CN
China
Prior art keywords
vibration
laser
resonance
polarization
birefringence
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
CN201810410240.7A
Other languages
Chinese (zh)
Other versions
CN108593089B (en
Inventor
张岳
李绪友
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to CN201810410240.7A priority Critical patent/CN108593089B/en
Publication of CN108593089A publication Critical patent/CN108593089A/en
Application granted granted Critical
Publication of CN108593089B publication Critical patent/CN108593089B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • 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

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

The invention discloses a kind of vibration of optical sensors and inducing method based on birefringence resonance effect.Vibration of optical sensor includes sequentially connected laser emission element, vibration induction amplifying unit, laser pick-off unit and reference waveform unit.The light that light source is sent out is modulated by laser emission element;Modulated optical signal is imported polarization-maintaining annular chamber by vibration induction amplifying unit, and optical signal resonance obtains two polarization eigen states;Laser pick-off unit converts optical signal into electric signal, and obtains the resonance demodulation curve and slope characteristics of two polarization eigen state ESOPs, and the induction of vibration is realized using the phase difference between two polarization states;Reference waveform unit carries out uniform modulation demodulation to transmission signal.The present invention is exaggerated susceptibility of the light to vibration using birefringence resonance effect, to realize high sensitivity, measure the big vibration induction of spatial dimension.

Description

A kind of vibration of optical sensor and inducing method based on birefringence resonance effect
Technical field
The present invention relates to a kind of vibrating sensor, specifically a kind of vibration of optical based on birefringence resonance effect passes Sensor and inducing method.
Background technology
In the past few decades, vibration of optical sensor is because of the features such as high sensitivity, big measurement spatial dimension, electromagnetism be insensitive And it is fast-developing.Existing vibration of optical sensor includes mainly distributed vibration sensor and point type vibrating sensor.Distribution Formula vibrating sensor is realized continuous vibration field measurement on an optical fiber, is had big based on the Rayleigh scattering effect in optical fiber The advantage that measures of spatial dimension, but sensitivity is poor, the vibration measurement not being suitable under highly sensitive and extreme environment.Point Although the spatial dimension that formula vibrating sensor measures is small, has outstanding vibration measurement ability.Two kinds of traditional optics shake Dynamic sensor is difficult to realize sensitivity and measures the balance between spatial dimension.
Invention content
In order to solve deficiency in the prior art, the present invention provides a kind of vibration of optical biography based on birefringence resonance effect Sensor is exaggerated susceptibility of the light to vibration using birefringence resonance effect, to realize that high sensitivity, measurement spatial dimension are big Vibration induction.
To achieve the goals above, the concrete scheme that the present invention uses for:
A kind of vibration of optical sensor based on birefringence resonance effect, a kind of optics based on birefringence resonance effect shake Dynamic sensor, including sequentially connected laser emission element, vibration induction amplifying unit, laser pick-off unit and reference waveform list Member;The laser emission element includes the laser and phase-modulator being connected with each other;The vibration induction amplifying unit includes The input terminal of polarization-maintaining annular chamber, polarization-maintaining annular chamber is connected by polarization maintaining optical fibre with the output end of the phase-modulator, and Tie point uses 45 ° of direction spin weldings;The laser pick-off unit includes sequentially connected photodetector, lock-in amplifier And signal processor, wherein photodetector are connected with the output end of the polarization-maintaining annular chamber, signal generator swashs with described Light device is connected;The reference waveform unit includes signal generator, signal generator and the phase-modulator and the lock Phase amplifier is connected.
As a preferred embodiment, the laser is connected by isolator with the phase-modulator.
As a preferred embodiment, the polarization-maintaining annular chamber has first input port, the second input port, the first output Port and second output terminal mouth, wherein the second input port and second output terminal mouth pass through 0 ° of welding reflection cyclization.
As a preferred embodiment, the output end of the phase-modulator is connected with the first input port.
As a preferred embodiment, the signal generator output sine wave or square wave.
As a preferred embodiment, the laser is set as the high coherent laser of narrow linewidth.
A kind of inducing method of the vibration of optical sensor based on birefringence resonance effect, includes the following steps:
S1, the laser export a laser and are transferred to the phase-modulator, while the signal generator sends out tune Waveform processed and demodulation waveforms are simultaneously transferred to phase-modulator;
S2, the phase-modulator are modulated according to the phase of a laser of modulation waveform pair, modulated laser export to The polarization-maintaining annular chamber;
S3, a laser play two ESOPs resonance with polarization eigen state in the polarization-maintaining annular chamber underexcitation;
S4, external vibration act on the difference on the polarization-maintaining annular chamber between the resonance point of two ESOPs resonance and generate shadow It rings, obtains secondary laser;
Secondary laser is transferred to the photodetector and the lock-in amplifier by S5, the polarization-maintaining annular chamber successively, simultaneously Demodulation waveforms are transferred to lock-in amplifier by the signal generator;
Secondary laser is demodulated to obtain electric signal and be amplified by lock-in amplifier, electric signal by S6, the photodetector Include the slope characteristics of two ESOPs resonance;
Amplified electric signal transmission is given the signal processor, signal processor to export two by S7, the lock-in amplifier Difference between ESOPs resonance, you can vibration information is obtained according to difference.
As a preferred embodiment, in the S7, the signal processor obtains the difference between two ESOPs resonance Method is:
Laser described in S7.1, signal processor output sawtooch sweep;
S7.2, the signal processor just obtain the slope characteristics of two ESOPs resonance from the lock-in amplifier;
S7.3, the signal processor calculate the difference between two ESOPs resonance according to the slope characteristics of two resonance.
As a preferred embodiment, in S7, the computational methods of vibration information areWherein, Δ A is vibration letter Breath, k0It is the wave number under vacuum, l is the length of transmission waveguide,It is the Oscillating Coefficients of birefringence difference, φ is the phase of resonance point Difference.
Advantageous effect:The present invention is two-fold to amplify and detect using the light resonance effect that multi-turn is transmitted in polarization-maintaining annular chamber Vibration is penetrated, to greatly improve the sensitivity to vibration.Two orthogonal polarization modes transmit in same waveguide, many Noise is because reciprocity (common mode) is eliminated, to realize the vibration detecting of high sensitivity.
Description of the drawings
Fig. 1 is the overall structure diagram of the present invention;
Fig. 2 is the structural schematic diagram of polarization-maintaining annular chamber of the present invention;
Fig. 3 is the resonance demodulation curve of two ESOPs in the present invention;
Fig. 4 is the resonance characteristic of two ESOPs and intracavitary transmits the relation schematic diagram that birefringence in one week differs, and birefringence difference is 0;
Fig. 5 is the resonance characteristic of two ESOPs and intracavitary transmits the relation schematic diagram that birefringence in one week differs, and birefringence difference is 0.5π;
Fig. 6 is the resonance characteristic of two ESOPs and intracavitary transmits the relation schematic diagram that birefringence in one week differs, and birefringence difference is π;
Fig. 7 is the resonance characteristic of two ESOPs and intracavitary transmits the relation schematic diagram that birefringence in one week differs, and birefringence difference is 1.5π;
Fig. 8 is that the difference between two resonance points transmits the relation schematic diagram that birefringence in one week differs, birefringence difference with intracavitary Range be 0~2 π;
Fig. 9 is that the difference between two resonance points transmits the relation schematic diagram that birefringence in one week differs, birefringence difference with intracavitary Range be 0~0.07 π.
Reference numeral:1, first input port, the 2, second input port, the 3, first output port, 4, second output terminal mouth, 5, coupler.
Specific implementation mode
Following will be combined with the drawings in the embodiments of the present invention, and technical solution in the embodiment of the present invention carries out clear, complete Site preparation describes, it is clear that described embodiments are only a part of the embodiments of the present invention, instead of all the embodiments.It is based on Embodiment in the present invention, it is obtained by those of ordinary skill in the art without making creative efforts every other Embodiment shall fall within the protection scope of the present invention.
Please refer to Fig.1 to 9, Fig. 1 be the present invention overall structure diagram, Fig. 2 is the structure of polarization-maintaining annular chamber of the present invention Schematic diagram, Fig. 3 are the resonance demodulation curves of two ESOPs in the present invention, and Fig. 4 is that the resonance characteristic of two ESOPs and intracavitary pass The relation schematic diagram of the defeated difference of birefringence in one week, birefringence difference are that 0, Fig. 5 is that the resonance characteristic of two ESOPs and intracavitary are transmitted The relation schematic diagram of the difference of birefringence in one week, birefringence difference are 0.5 π, and Fig. 6 is that the resonance characteristic of two ESOPs and intracavitary pass The relation schematic diagram of the defeated difference of birefringence in one week, birefringence difference are π, and Fig. 7 is that the resonance characteristic of two ESOPs and intracavitary are transmitted The relation schematic diagram of the difference of birefringence in one week, birefringence difference are 1.5 π, and Fig. 8 is that the difference between two resonance points is passed with intracavitary The relation schematic diagram of the defeated difference of birefringence in one week, the range of birefringence difference is 0~2 π, and Fig. 9 is the phase between two resonance points Difference transmits the relation schematic diagram that birefringence in one week differs with intracavitary, and the range of birefringence difference is 0~0.07 π.
A kind of vibration of optical sensor based on birefringence resonance effect, including sequentially connected laser emission element, shake Innervation answers amplifying unit, laser pick-off unit and reference waveform unit.
The sequentially connected laser of laser emission element, isolator and phase-modulator, laser are set as narrow linewidth High coherent laser can be specifically YAG laser, gas laser, semiconductor laser or optical fiber laser, laser It is connected with phase-modulator by isolator.
Vibration induction amplifying unit includes polarization-maintaining annular chamber, and polarization-maintaining annular chamber has first input port 1, the second input terminal The 2, first output port 3 of mouth and second output terminal mouth 4, wherein the second input port 2 and second output terminal mouth 4 are anti-by 0 ° of welding Penetrate cyclization.The first input port 1 of polarization-maintaining annular chamber is connected by polarization maintaining optical fibre with the output end of phase-modulator, and even Contact uses 45 ° of direction spin weldings.
Laser pick-off unit includes sequentially connected photodetector, photodetector and signal processor, wherein photoelectricity Detector is connected with the output end of polarization-maintaining annular chamber, and signal generator is connected with laser.
Reference waveform unit includes signal generator, and signal generator is connected with phase-modulator and photodetector, The reference waveform of signal generator output is sine wave or square wave.
All devices can integration realization on the semiconductor, discrete component combination can also be passed through and realized.
Based on above-mentioned vibration of optical sensor, the present invention also provides a kind of, and the vibration of optical based on birefringence resonance effect passes The inducing method of sensor, including S1~S7.
S1, laser export a laser simultaneously be transferred to phase-modulator, synchronous signal generator send out modulation waveform and Demodulation waveforms are simultaneously transferred to phase-modulator.
S2, phase-modulator are modulated according to the phase of a laser of modulation waveform pair, modulated laser export to Polarization-maintaining annular chamber.
S3, a laser play two resonance with polarization eigen state in polarization-maintaining annular chamber underexcitation.
S4, external vibration act on the difference on polarization-maintaining annular chamber between the resonance point of two ESOPs resonance and generate shadow It rings, obtains secondary laser.
Secondary laser is transferred to photodetector and lock-in amplifier by S5, polarization-maintaining annular chamber successively, and synchronous signal occurs Demodulation waveforms are transferred to lock-in amplifier by device.
Secondary laser is demodulated to obtain electric signal and be amplified by lock-in amplifier, electric signal by S6, photodetector Include the slope characteristics of two ESOPs resonance.
By amplified electric signal transmission to signal processor, signal processor exports two ESOPs for S7, lock-in amplifier Between difference, you can according to difference obtain vibration information.The computational methods of vibration information areWherein, Δ A It is vibration information, k0It is the wave number under vacuum, l is the length of transmission waveguide,It is the Oscillating Coefficients of birefringence difference, φ is humorous The difference shaken a little.
The method that specific signal processor obtains differing between the resonance point of two ESOPs resonance include S7.1~ S7.3。
S7.1, signal processor export sawtooch sweep laser.
S7.2, signal processor just obtain the slope characteristics of two ESOPs from lock-in amplifier.
S7.3, signal processor calculate the difference between two ESOPs according to the slope characteristics of two resonance.
Working principle of the present invention is as follows.
First, a laser is input to from first input port 1 in polarization-maintaining annular chamber, then by after coupler 5 from Two output ports 4 enter in polarization-maintaining annular chamber, and the matrix transmitted one week in polarization-maintaining annular chamber is:
Wherein, α is the loss that light transmits one week in intracavitary, it includes mainly the transmission loss and coupler of optical waveguide Insertion loss;K is the coefficient of coup;β and Δ β is that the propagation constant that average propagation constant and birefringence introduce is poor respectively;θt Equivalent theta alignment error is indicated, for describing the polarization interference at the straight-through end of coupler;L is the length of wave guide ring shaped resonant cavity Degree.
Characteristic value λmWith eigenvector vmIt is 2 key parameters of matrix S, they meet
Svmmvm(m=1,2); (2)
Wherein, eigenvector vmIllustrate such polarization state:Light is passed since the second output terminal mouth 4 of coupler 5 in intracavitary Defeated polarization state is restored to the state set out after a week, and here it is the polarization eigen state ESOPs that we often say;And characteristic value λmTable The transmission coefficient that ESOPs resonance transmits one week in intracavitary, characteristic value λ are shownmIt is a plural number, and non-matrix, thus significantly Reduce the difficulty of polarization analysis.
Characteristic value λ can be obtained by formula (1) and formula (2)mComputational methods:
Wherein, ξ meets:
In general, the polarization extinction of waveguide coupler is higher, i.e. θtIt is smaller, therefore work as Δ βl< θtWhen, above formula (4) It can be reduced to:
Assuming that the light field of a laser is E1, is injected from the first input port 1 of coupler 5, be then coupled to second The light field of output port 4, outgoing is E4, is projected to respectively on two ESOPs:
Wherein, a, b are the amplitude of polarization eigen state v1 and v2 respectively;V is the combinatorial matrix of ESOPs, V=(ν 1, ν 2);CkIt is coupling Close matrix:
Wherein, θkFor describing the equivalent angles alignment error that coupler intersects end.
Incident light is transmitted in intracavitary multi-turn, and the cumulative light field of 2 ESOPs is respectively:
By formula (8) and formula (3) it is found that intracavitary will encourage two resonance states, and the difference of resonance point is:
The ξ of φ=2.(9)
By formula (5) it is found that working as Δ βl> > θtWhen,
φ=Δ β l.(10)
By formula (10) it is found that the birefringence that the difference of two resonance points, which is exactly polarization-maintaining annular chamber, to be transmitted one week differs.
When vibrating variation, the birefringence dither effect of polarization-maintaining optical waveguide is as follows:
Wherein, Δ A is vibration information, k0It is the wave number under vacuum, l is the length of transmission waveguide,It is shaking for birefringence difference Dynamic coefficient.Therefore, by detecting the difference (birefringence difference) of two resonance points, vibration can be detected:
According to above-mentioned theory analysis, emulation obtains resonance characteristic and transmits the relationship such as figure that birefringence in one week differs with intracavitary Shown in 4 to 7.In order to encourage the resonance of 2 ESOPs, linearly polarized light to be incident on polarization-maintaining with slow axis direction at 45 ° simultaneously in intracavitary Annular chamber.When the birefringence difference that intracavitary is transmitted one week is zero, the resonance of two ESOPs is in close proximity, with the increasing of difference Greatly, the distance between two resonance points also increase therewith.
The relationship that difference between two resonance points is differed with intracavitary transmission birefringence in one week is as shown in FIG. 8 and 9.When two-fold Penetrate difference it is larger (>0.1 π rad) when, the approximately linear relationship of the two, this region can be used to measure the variation of vibration;But when double Refraction difference it is smaller when, the two is not linear, the difference between two resonance points with the reduction that birefringence differs and It is intended to 2 θt, this region is unable to measure the variation of vibration.
The present invention is amplified using the light resonance effect that multi-turn is transmitted in the polarization-maintaining annular chamber of annular and detects birefringence Vibration to greatly improve the sensitivity of vibration, and is realized continuous vibration field measurement on an optical fiber, is measured empty Between range it is big.Two orthogonal polarization modes transmit in same waveguide, and many noises are because reciprocity (common mode) is eliminated, to real The vibration detecting of existing high sensitivity.
It should also be noted that, herein, relational terms such as first and second and the like are used merely to one Entity or operation are distinguished with another entity or operation, without necessarily requiring or implying between these entities or operation There are any actual relationship or orders.Moreover, the terms "include", "comprise" or its any other variant are intended to contain Lid non-exclusive inclusion, so that the process, method, article or equipment including a series of elements is not only wanted including those Element, but also include other elements that are not explicitly listed, or further include for this process, method, article or equipment Intrinsic element.In the absence of more restrictions, the element limited by sentence "including a ...", it is not excluded that There is also other identical elements in process, method, article or equipment including the element.
The foregoing description of the disclosed embodiments enables those skilled in the art to implement or use the present invention. Various modifications to these embodiments will be apparent to those skilled in the art, as defined herein General Principle can be realized in other embodiments without departing from the spirit or scope of the present invention.Therefore, of the invention It is not intended to be limited to the embodiments shown herein, and is to fit to and the principles and novel features disclosed herein phase one The widest range caused.

Claims (9)

1. a kind of vibration of optical sensor based on birefringence resonance effect, it is characterised in that:It is sent out including sequentially connected laser Penetrate unit, vibration induction amplifying unit, laser pick-off unit and reference waveform unit;
The laser emission element includes the laser and phase-modulator being connected with each other;
The vibration induction amplifying unit includes polarization-maintaining annular chamber, and the input terminal of polarization-maintaining annular chamber passes through polarization maintaining optical fibre and the phase The output end of position modulator is connected, and tie point uses 45 ° of direction spin weldings;
The laser pick-off unit includes sequentially connected photodetector, lock-in amplifier and signal processor, wherein photoelectricity Detector is connected with the output end of the polarization-maintaining annular chamber, and signal generator is connected with the laser;
The reference waveform unit includes signal generator, signal generator and the phase-modulator and the lock-in amplifier It is connected.
2. a kind of vibration of optical sensor based on birefringence resonance effect as described in claim 1, it is characterised in that:It is described Laser is connected by isolator with the phase-modulator.
3. a kind of vibration of optical sensor based on birefringence resonance effect as described in claim 1, it is characterised in that:It is described Polarization-maintaining annular chamber has first input port (1), the second input port (2), the first output port (3) and second output terminal mouth (4), wherein the second input port (2) and second output terminal mouth (4) pass through 0 ° of welding reflection cyclization.
4. a kind of vibration of optical sensor based on birefringence resonance effect as claimed in claim 3, it is characterised in that:It is described The output end of phase-modulator is connected with the first input port (1).
5. a kind of vibration of optical sensor based on birefringence resonance effect as described in claim 1, it is characterised in that:It is described Signal generator exports sine wave or square wave.
6. a kind of vibration of optical sensor based on birefringence resonance effect as described in claim 1, it is characterised in that:It is described Laser is set as the high coherent laser of narrow linewidth.
7. a kind of inducing method of the vibration of optical sensor based on birefringence resonance effect as described in claim 1, special Sign is:Include the following steps:
S1, the laser export a laser and are transferred to the phase-modulator, while the signal generator sends out tune Waveform processed and demodulation waveforms are simultaneously transferred to phase-modulator;
S2, the phase-modulator are modulated according to the phase of a laser of modulation waveform pair, modulated laser export to The polarization-maintaining annular chamber;
S3, a laser play two ESOPs resonance with polarization eigen state in the polarization-maintaining annular chamber underexcitation;
S4, external vibration act on the difference on the polarization-maintaining annular chamber between the resonance point of two ESOPs resonance and generate shadow It rings, obtains secondary laser;
Secondary laser is transferred to the photodetector and the lock-in amplifier by S5, the polarization-maintaining annular chamber successively, simultaneously Demodulation waveforms are transferred to lock-in amplifier by the signal generator;
Secondary laser is demodulated to obtain electric signal and be amplified by lock-in amplifier, electric signal by S6, the photodetector Include the slope characteristics of two ESOPs resonance;
Amplified electric signal transmission is given the signal processor, signal processor to export two by S7, the lock-in amplifier Difference between ESOPs resonance, you can vibration information is obtained according to difference.
8. inducing method as claimed in claim 6, it is characterised in that:In the S7, the signal processor obtains two The method of difference between ESOPs resonance is:
Laser described in S7.1, signal processor output sawtooch sweep;
S7.2, the signal processor just obtain the slope characteristics of two ESOPs resonance from the lock-in amplifier;
S7.3, the signal processor calculate the difference between two ESOPs resonance according to the slope characteristics of two resonance.
9. inducing method as claimed in claim 6, it is characterised in that:In S7, the computational methods of vibration information areWherein, Δ A is vibration information, k0It is the wave number under vacuum, l is the length of transmission waveguide,It is birefringence The Oscillating Coefficients of difference, φ are the difference of resonance point.
CN201810410240.7A 2018-05-02 2018-05-02 Optical vibration sensor based on birefringence resonance effect and sensing method Active CN108593089B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201810410240.7A CN108593089B (en) 2018-05-02 2018-05-02 Optical vibration sensor based on birefringence resonance effect and sensing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201810410240.7A CN108593089B (en) 2018-05-02 2018-05-02 Optical vibration sensor based on birefringence resonance effect and sensing method

Publications (2)

Publication Number Publication Date
CN108593089A true CN108593089A (en) 2018-09-28
CN108593089B CN108593089B (en) 2020-08-04

Family

ID=63619577

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201810410240.7A Active CN108593089B (en) 2018-05-02 2018-05-02 Optical vibration sensor based on birefringence resonance effect and sensing method

Country Status (1)

Country Link
CN (1) CN108593089B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110895165A (en) * 2019-12-27 2020-03-20 华中科技大学 Optical fiber vibration sensing system based on polarization maintaining optical fiber

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20100004318A (en) * 2008-07-03 2010-01-13 창원대학교 산학협력단 Depolarized fiber-optic gyroscope
CN103528666A (en) * 2013-09-29 2014-01-22 中国电子科技集团公司第四十一研究所 Long-distance optical fiber vibration detection device and method on basis of Sagnac interference
US20140218739A1 (en) * 2008-02-14 2014-08-07 Ralph A. Bergh Interferometer employing a multi-waveguide optical loop path and fiber optic rotation rate sensor employing same
CN104121983A (en) * 2014-07-14 2014-10-29 南京林业大学 Birefringence optical fiber environment based vibration dynamic monitoring system and method
US20150369605A1 (en) * 2014-06-23 2015-12-24 Honeywell International Inc. Symmetric three-laser resonator fiber optic gyroscope
WO2016135289A1 (en) * 2015-02-27 2016-09-01 Nils Schopohl Sensor device for tires
CN106200015A (en) * 2016-08-01 2016-12-07 天津理工大学 Microwave photon filter based on high double-refraction photon crystal fiber multiple-wavelength laser Yu dispersion cascode device

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20140218739A1 (en) * 2008-02-14 2014-08-07 Ralph A. Bergh Interferometer employing a multi-waveguide optical loop path and fiber optic rotation rate sensor employing same
KR20100004318A (en) * 2008-07-03 2010-01-13 창원대학교 산학협력단 Depolarized fiber-optic gyroscope
CN103528666A (en) * 2013-09-29 2014-01-22 中国电子科技集团公司第四十一研究所 Long-distance optical fiber vibration detection device and method on basis of Sagnac interference
US20150369605A1 (en) * 2014-06-23 2015-12-24 Honeywell International Inc. Symmetric three-laser resonator fiber optic gyroscope
CN104121983A (en) * 2014-07-14 2014-10-29 南京林业大学 Birefringence optical fiber environment based vibration dynamic monitoring system and method
WO2016135289A1 (en) * 2015-02-27 2016-09-01 Nils Schopohl Sensor device for tires
CN106200015A (en) * 2016-08-01 2016-12-07 天津理工大学 Microwave photon filter based on high double-refraction photon crystal fiber multiple-wavelength laser Yu dispersion cascode device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110895165A (en) * 2019-12-27 2020-03-20 华中科技大学 Optical fiber vibration sensing system based on polarization maintaining optical fiber
CN110895165B (en) * 2019-12-27 2021-09-24 华中科技大学 Optical fiber vibration sensing system based on polarization maintaining optical fiber

Also Published As

Publication number Publication date
CN108593089B (en) 2020-08-04

Similar Documents

Publication Publication Date Title
US5046848A (en) Fiber optic detection system using a Sagnac interferometer
US6798523B2 (en) Sensor and method for detecting fiber optic faults
CN100437050C (en) Distribution type fiber-optic vibration sensor
JP7401548B2 (en) Distributed sensing device
CN110108346A (en) Optical fibre vibration sensor based on delay phase modulation chirped pulse pair
CN110319828A (en) A kind of the resonance type optical fiber gyro system and its signal detecting method of bicyclic cavity configuration
AU2002364176A1 (en) Symmetrical depolarized fiber optic gyroscope
CN109752581A (en) Polarize analyzing formula closed loop all-fiber current transformator
CN108593089A (en) A kind of vibration of optical sensor and inducing method based on birefringence resonance effect
CN109831249A (en) A kind of measuring device of polarization maintaining optical fibre main shaft difference delay
CN111486939B (en) Ultrasonic measuring device for realizing optical path and polarization state regulation and control based on SAGNAC principle
CN106597061A (en) Sagnac type fiber current sensor and current detection method thereof
JP4599560B2 (en) Reference signal light transmission system and reference signal light transmission method
CN108180978A (en) A kind of combination PGC technologies and the method and device of Φ-OTDR technique detection optical fiber vibration
WO2002066940A3 (en) System and method for measurement of the state of polarization of an optical signal in a fibre
CN201749141U (en) Full fiber current transformer
CN104459350B (en) A kind of lithium niobate straight wave guide electric field measurement system
JPH02118416A (en) Optical sensor
CN104180970A (en) Polarization characteristic testing method and device for basic-unit structure parameters of polarization-maintaining optical-waveguide annular resonant cavity
JP2005214892A (en) Electric field sensor and electric field detection method
CN209102100U (en) A kind of detection device
CN110186501A (en) A kind of non-equilibrium fibre optic interferometer arm length difference measuring device and measuring method using comparison method
CN211262664U (en) Measuring device for mode birefringence of high-birefringence polarization maintaining optical fiber
JPS63106707A (en) Optical signal processing method and optical system
Mi et al. A self‐tracking phase retrieval algorithm used in distributed disturbance sensing

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