CN206673311U - Optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect - Google Patents

Optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect Download PDF

Info

Publication number
CN206673311U
CN206673311U CN201720152650.7U CN201720152650U CN206673311U CN 206673311 U CN206673311 U CN 206673311U CN 201720152650 U CN201720152650 U CN 201720152650U CN 206673311 U CN206673311 U CN 206673311U
Authority
CN
China
Prior art keywords
signal
brillouin scattering
laser
optical
effect
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.)
Expired - Fee Related
Application number
CN201720152650.7U
Other languages
Chinese (zh)
Inventor
吴帆
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.)
Yangcheng Institute of Technology
Original Assignee
Yangcheng Institute 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 Yangcheng Institute of Technology filed Critical Yangcheng Institute of Technology
Priority to CN201720152650.7U priority Critical patent/CN206673311U/en
Application granted granted Critical
Publication of CN206673311U publication Critical patent/CN206673311U/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Abstract

The utility model provides a kind of optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect, it is related to field of photoelectric technology, it includes first laser device, circulator, fiber unit, second laser, phase-modulator, tunable attenuator, photodetector unit, tunable filter, coupler and electric amplifier.Wherein, the multiple-frequency signal as caused by the laser that the second laser exports through the phase-modulator, with the laser signal caused generation of the brillouin scattering signal backwards stimulated Brillouin scattering amplification in fiber unit exported by the first laser device, exaggerated multiple-frequency signal is divided into two paths of signals by coupler again through decay, opto-electronic conversion and filtering, signal exports as feedback signal input phase modulator, another way signal as microwave signal all the way.The utility model is by changing the output wavelength of first laser device, and then the frequency for changing feedback signal finally realizes tunable microwave signal output to obtain required multiple-frequency signal.

Description

Optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect
Technical field
Field of photoelectric technology is the utility model is related to, in particular to one kind based on stimulated Brillouin scattering amplification effect The optical-electronic oscillator answered.
Background technology
At present, adjustable microwave signal source is that satellite communication system, radar system and sensor-based system etc. are necessary and important Signal source.With the high speed development of information technology and increasing sharply for data transmission service, to the bandwidth requirement of signal source with Increase.Compared with traditional microwave signal source, optical-electronic oscillator has larger advantage in terms of high-frequency signal generation, and believes Number there is relatively low phase noise, therefore, cause the great attention of researcher.
Part researcher utilizes the stimulated Brillouin scattering effect in optical fiber, and single sideband modulation light in optical-electronic oscillator is believed Number carrier wave carry out phase shift, by by the carrier wave of light modulating signal and positive single order sideband or carrier wave with negative one rank sideband in optical detection Beat frequency at device, realizes the change of microwave signal phase-shift phase in optical-electronic oscillator annular chamber, while coordinates adjustable microwave wave filter, The final broadband continuously adjustable for realizing optical-electronic oscillator output signal frequency.
It is another to have part researcher defeated using the tunable microwave signal of microwave source shift frequency combination optical fiber Brillouin effect acquisition Go out.
Newest result of study is, by the use of silica-based waveguides as the energy-storage travelling wave tube of oscillator, to produce be excited cloth in the waveguide In deep scattering effect, with reference to light injection distributed feedback laser carry out shift frequency, by change temperature control system temperature and swash The wavelength of light device realizes the tunability of output microwave signal.
The above achievement in research has certain practicality in terms of the generation of microwave signal, achieves and certain enters Exhibition.But be all the laser used in the scheme reported at present, it is micro- that the tuning property of the laser limits output The tuning performance of ripple signal, limit the application of these optical-electronic oscillator microwave signal sources.
Utility model content
The purpose of this utility model is to provide a kind of optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect, its Above mentioned problem can effectively be improved.
What embodiment of the present utility model was realized in:
The utility model embodiment provides a kind of optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect, and it is wrapped Include first laser device, circulator, fiber unit, second laser, phase-modulator, tunable attenuator, photodetector list Member, tunable filter, coupler and electric amplifier;Enter from the light beam of first laser device output by the circulator The fiber unit, and produced in the fiber unit backwards to brillouin scattering signal;From second laser output Light beam forms multiple-frequency signal by the phase modulator modulation and enters the fiber unit, in the multiple-frequency signal with the back of the body Carried on the back to brillouin scattering signal frequency identical signal in the fiber unit with the brillouin scattering signal backwards To Brillouin scattering enlarge-effect, its power is exaggerated;Exaggerated multiple-frequency signal enters described adjustable by the circulator Humorous attenuator, the multiple-frequency signal after the tunable attenuator decay are converted to electric signal through the photodetector unit; The electric signal filters by the tunable filter, then is divided into two paths of signals by the coupler, wherein signal is made all the way Enter the phase-modulator by electric amplifier amplification for feedback signal, another way signal exports as microwave signal.
In the utility model preferred embodiment, the first laser device is wavelength and the tunable laser of power Device.
In the utility model preferred embodiment, the second laser is wavelength and the tunable narrow linewidth of power Laser.
In the utility model preferred embodiment, the second laser is the narrow linewidth laser of fixed wave length.
In the utility model preferred embodiment, the fiber unit is single-mode fiber.
In the utility model preferred embodiment, the fiber unit is dispersion shifted optical fiber.
In the utility model preferred embodiment, the fiber unit is highly nonlinear optical fiber.
In the utility model preferred embodiment, the fiber unit is the highly nonlinear optical fiber that length is 5km.
In the utility model preferred embodiment, the photodetector unit is photodetector.
In the utility model preferred embodiment, the photodetector unit is balanced detector.
Relative in the prior art only using a laser output laser signal and direct by being carried out to laser signal Modulate to export the optical-electronic oscillator of microwave signal, what the utility model embodiment provided amplifies effect based on stimulated Brillouin scattering The optical-electronic oscillator answered using brillouin scattering signal can amplify with its frequency identical signal characteristic, with reference to phase-modulator Multiple-frequency signal and the low noise feature of optical-electronic oscillator can be produced, by setting first laser device and second laser, make by The laser of the second laser output is through multiple-frequency signal caused by the phase-modulator, with being exported by the first laser device Laser signal in fiber unit caused by backwards to brillouin scattering signal occur stimulated Brillouin scattering amplification, by amplification Multiple-frequency signal afterwards is divided into two paths of signals further across decay, opto-electronic conversion and filtering, then by coupler, wherein signal all the way As feedback signal input phase modulator, another way signal exports as microwave signal.By setting feedback circuit so that only The output wavelength of first laser device need to be adjusted, you can change the frequency backwards to brillouin scattering signal, and then change multiple-frequency signal In with the signal frequency of stimulated Brillouin scattering amplification occurs backwards to brillouin scattering signal, then amplified by feedback circuit Feedback signal afterwards and input phase modulator, change the frequency distribution of the multiple-frequency signal of phase-modulator output, thus may be used A certain frequency signal in the multiple-frequency signal exported with the amplification of selectivity from phase-modulator, finally obtains tunable microwave Signal output.Therefore, optical-electronic oscillator provided by the utility model can not only produce High-precision Microwave signal, and can obtain The microwave signal with wide tunable is obtained, and phase-modulation is carried out by feedback circuit, the external equipment of costliness is eliminated, simplifies The structure of optical-electronic oscillator, reduces volume, saves cost, greatly reduces electromagnetic interference, makes adjustable microwave signal Acquisition becomes more simple.
Brief description of the drawings
, below will be to required use in embodiment in order to illustrate more clearly of the technical scheme of the utility model embodiment Accompanying drawing be briefly described, it will be appreciated that the following drawings illustrate only some embodiments of the present utility model, therefore should not be by Regard the restriction to scope as, for those of ordinary skill in the art, on the premise of not paying creative work, may be used also To obtain other related accompanying drawings according to these accompanying drawings.
Fig. 1 is the optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect in the utility model first embodiment Structural representation;
Fig. 2 is the multiple-frequency signal spectrum that phase-modulator exports in the utility model first embodiment;
Fig. 3 is the spectrum diagram of the microwave signal that optical-electronic oscillator exports in the utility model first embodiment;
Fig. 4 is the spectrum diagram of the microwave signal of the continuously adjustable obtained in the utility model first embodiment.
Icon:100- first laser devices;110- circulators;120- fiber units;130- second lasers;140- phases are adjusted Device processed;150- is tunable attenuator;160- photodetector units;170- tunable filters;180- couplers;190- is electrically amplified Device;Optical-electronic oscillators of the 1000- based on stimulated Brillouin scattering enlarge-effect.
Embodiment
It is new below in conjunction with this practicality to make the purpose, technical scheme and advantage of the utility model embodiment clearer Accompanying drawing in type embodiment, the technical scheme in the embodiment of the utility model is clearly and completely described, it is clear that is retouched The embodiment stated is the utility model part of the embodiment, rather than whole embodiments.Generally here described in accompanying drawing and The component of the utility model embodiment shown can be configured to arrange and design with a variety of.
Therefore, the detailed description of the embodiment of the present utility model to providing in the accompanying drawings is not intended to limit requirement below The scope of the utility model of protection, but it is merely representative of selected embodiment of the present utility model.Based in the utility model Embodiment, the every other embodiment that those of ordinary skill in the art are obtained under the premise of creative work is not made, all Belong to the scope of the utility model protection.
It should be noted that:Similar label and letter represents similar terms in following accompanying drawing, therefore, once a certain Xiang Yi It is defined, then it further need not be defined and explained in subsequent accompanying drawing in individual accompanying drawing.
, it is necessary to explanation in description of the present utility model, term " in ", " on ", " under ", "left", "right", " interior ", The orientation or position relationship of instructions such as " outer " are or the utility model product based on orientation shown in the drawings or position relationship The orientation or position relationship usually put during use, it is for only for ease of description the utility model and simplifies description, without referring to Show or imply that the device of meaning or element there must be specific orientation, with specific azimuth configuration and operation, therefore can not manage Solve as to limitation of the present utility model.In addition, term " first ", " second ", " the 3rd " etc. are only used for distinguishing description, and can not manage Solve to indicate or implying relative importance.
In addition, the term such as term " level ", " vertical ", " pendency " is not offered as requiring part abswolute level or pendency, and It is to be slightly tilted.Such as " level " only refers to that its direction is more horizontal with respect to for " vertical ", is not to represent the structure Must be fully horizontal, but can be slightly tilted.
In description of the present utility model, it is also necessary to which explanation, unless otherwise clearly defined and limited, term " are set Put ", " installation ", " connected ", " connection " should be interpreted broadly, for example, it may be fixedly connected or be detachably connected, Or it is integrally connected;Can be mechanical connection or electrical connection;Can be joined directly together, intermediary can also be passed through It is indirectly connected, can is the connection of two element internals.For the ordinary skill in the art, can be managed with concrete condition Solve concrete meaning of the above-mentioned term in the utility model.
In addition, the term such as " input ", " output ", " feedback ", " formation " is understood as describing a kind of optics, electricity change Or optics, electricity processing.As " is formationed " only refer to optical signal or electric signal by the element, instrument or device afterwards there occurs Change optically or electrically so that the optical signal or the electric signal are processed, and then are obtained and implemented technical scheme Or the signal required for solution technical problem.
In specific embodiment of the utility model accompanying drawing, for more preferable, clearer description each element of optical-electronic oscillator Operation principle, show described device in each several part annexation, simply substantially distinguished the relative position between each element Relation, it can not form to the optical path direction in element or structure, the order of connection and Each part size, size, shape Limit.
First embodiment
Fig. 1 is refer to, the present embodiment provides a kind of optical-electronic oscillator 1000 based on stimulated Brillouin scattering enlarge-effect, It includes first laser device 100, circulator 110, fiber unit 120, second laser 130, phase-modulator 140, tunable Attenuator 150, photodetector unit 160, tunable filter 170, coupler 180 and electric amplifier 190.
In the present embodiment, the first laser device 100 is wavelength and the tunable Agilent narrow line width regulatable of power Laser (Agilent lightwave measurement system8164B), its output wavelength scope be 1527.60~ 1565.5nm, output power range are -13~6dBm.In the present embodiment, the output wavelength of the first laser device 100 is set in 1550nm, power output are set as 5dBm.
In the present embodiment, it is respectively A ports, B ports and C-terminal mouth that the circulator 110, which has three ports, and its signal passes Defeated direction is counterclockwise transmission.It is understood that enter the signal of circulator 110 from the B ports from the A ports Output, the signal that circulator 110 is entered from the B ports export from the C-terminal mouth.
In the present embodiment, the circulator 110 passes through the B ports and the optical coupling of fiber unit 120.Swash from described first The narrow-linewidth laser signal that light device 100 exports inputs from the A ports of circulator 110, is passed in circulator 110 through counter clockwise direction It is defeated to export and enter in fiber unit 120 from the B ports of circulator 110.Into the laser signal in fiber unit 120 in optical fiber Produced in unit 120 backwards to brillouin scattering signal, the transmission direction backwards to brillouin scattering signal and former laser signal It is in opposite direction.
It is due to that there occurs stimulated Brillouin scattering in fiber unit 120 for laser signal backwards to brillouin scattering signal (Stimulated Brillouin Scattering, SBS) effect and it is caused.Due to entering the laser in fiber unit 120 The power of signal is very high, and it generates highfield in inside of optical fibre, by the way that electrostriction effect occurs so that fiber medium occurs The change of periodic density and dielectric constant, and then acoustic wavefield is generated, so as to causing incident laser signal and acoustic wavefield Between there occurs coherent scattering, that is, generate stimulated Brillouin scattering signal, its direction of propagation and former laser signal are on the contrary, therefore Referred to as backwards to brillouin scattering signal.
In the present embodiment, the fiber unit 120 is the general single mode fiber that length is 21km, the common list of such length Mode fiber can strengthen the excited Brillouin occurred by the laser signal that first laser device 100 exports in fiber unit 120 and dissipate Penetrate effect.
In the present embodiment, the second laser 130 is wavelength and the tunable Agilent narrow line width regulatable of power Laser (N7714A multichannels narrow linewidth laser), its output wavelength scope are 1527.60~1565.5nm, power output model Enclose for -10~14dBm.In the present embodiment, the output wavelength of second laser 130 is arranged to 1550nm, and power output is arranged to 10dBm。
In the present embodiment, the phase-modulator 140 is Photline 1550nm wave bands lithium niobate (LiNbO3) electric light phase Position modulator 140, model MPZ-LN-20, it can be by carrying out phase-modulation to export by certain by single-frequency input signal The multiple-frequency signal of frequency interval distribution.
In the present embodiment, the output end of the phase-modulator 140 and the optical coupling of fiber unit 120.By described The narrow-linewidth laser signal that dual-laser device 130 exports inputs from the optical signal input of phase-modulator 140, phase modulated device 140 multiple-frequency signals of the modulation output with certain frequency interval.The multiple-frequency signal enters in fiber unit 120, with the back of the body Interacted to brillouin scattering signal so that the power of multiple-frequency signal is exaggerated.
On say multiple-frequency signal with backwards to brillouin scattering signal interaction be based on stimulated Brillouin scattering effect in Enlarge-effect.When heavy pumping laser signal field is incided in fiber unit 120, the electrostriction effect of light wave fields has started Effect, is greatly enhanced the acoustic frequency vibration (phonon) of some states in fiber optic materials medium, and the acoustic wavefield enhanced is again anti- Come over scattering process of the enhancing to incident laser, acoustic wavefield, the laser wave field (laser signal and phase that first laser device 100 exports The multiple-frequency signal that position modulator 140 exports), the scattering light wave fields (backwards to brillouin scattering signal) of laser deposits simultaneously in media as well It is being mutually coupled.After the intensity of incident laser reaches threshold value, make acoustic wavefield and the humidification foot of scattering light wave fields in medium To compensate respective loss effect, being excited to amplify or vibrating effect for sensing acoustic wavefield and Brillouin scattering light wave fields can be now produced Should.
It is understood that in the present embodiment, into the multiple-frequency signal in fiber unit 120, frequency and the back of the body It can be put to brillouin scattering signal frequency identical signal with described backwards to brillouin scattering signal generation stimulated Brillouin scattering Big effect, the signal switch to the energy backwards to brillouin scattering signal for amplification after signal energy, i.e. multiple-frequency signal Overall power be exaggerated.
Because the frequency displacement of stimulated Brillouin scattering penetrates the ratio of optical frequency less than 10 with people-6, and believe backwards to Brillouin scattering Number intensity it is very weak.Therefore in order to strengthen stimulated Brillouin scattering effect, high power, narrow linewidth have all been selected in the present embodiment Signal source and high sensitivity, high-precision detector.
Multiple-frequency signal by stimulated Brillouin scattering amplification enters the B ports of circulator 110, by the C-terminal of circulator 110 Enter tunable attenuator 150 after mouth output.In the present embodiment, because the multiple-frequency signal power after amplification is very high, exceed The detection range of photodetector unit 160, it is therefore desirable to tunable attenuator is added before photodetector unit 160 150, power attenuation is carried out to the multiple-frequency signal by amplification.Due to the part only output in need being exaggerated in multiple-frequency signal The part signal of frequency, signal (noise) power of other frequencies is not high, while power attenuation is carried out, also filters out Partial noise.
In the present embodiment, the transmission photodetector unit is 50GHz Finisar XPDV21x0RA photodetectors, and it rings It is 1528~1564nm to answer wave-length coverage.Multiple-frequency signal after decaying by tunable attenuator 150 is by photodetector list The input input of member 160, is converted to the input that electric signal enters tunable filter 170.
In the present embodiment, the model Santec OTF-300 of tunable filter 170, its wave-length coverage be 1530~ 1570nm, with a width of 0.3nm.Tunable filter 170 filters out unwanted frequency in multiple-frequency signal, and required for exporting The signal of frequency (by the frequency of stimulated Brillouin scattering amplification), the signal enter in coupler 180 and are divided into two paths of signals Output.Wherein, signal is amplified as feedback signal into the input of electric amplifier 190 all the way, the feedback letter after amplification Number inputted by the electric signal input end mouth of phase-modulator 140, for drive phase-modulator 140 produce needed for frequency interval Multiple-frequency signal;And the another way electric signal that coupler 180 exports exports as microwave signal.
Because the multiple-frequency signal by initial phase modulation is possible to and does not have required frequency interval, therefore without Cross feedback modulation output microwave signal be also possible to be not required frequency interval microwave signal.Now pass through regulation first The output wavelength of laser 100, you can the corresponding frequency backwards to brillouin scattering signal changed in fiber unit 120, so that it may To drive phase-modulator 140 to produce required frequency signal.Dimension, tunable microwave signal output can be obtained.
Fig. 2 is refer to, the frequency spectrum of the multiple-frequency signal specifically exported from phase-modulator 140 is as shown in Figure 2.Can be with from Fig. 2 Find out, in the range of 10MHz, multiple-frequency signal there are 5 signal frequencies, and such multiple-frequency signal is established for the tuning performance of microwave signal Fixed basis.
Fig. 3 is refer to, the microwave signal spectrogram of the single-frequency exported by coupler 180 is as shown in Figure 3.Can from Fig. 3 To find out, the centre frequency of microwave signal is 22.05GHz.
Fig. 4 is refer to, when changing the output wavelength of first laser device 100, the frequency spectrum of the adjustable microwave signal of output Figure is as shown in Figure 4.From fig. 4, it can be seen that the microwave signal of output continuously adjustabe in the range of 0~40GHz, can so recognize To obtain tunable microwave signal output.
In the present embodiment, selected first laser device 100 and second laser 130 are all tunable for wavelength and power Narrow linewidth laser, relative to common tunable laser, its output frequency is stable, monochromaticjty is strong and noise is low, as Signal source can make that optical-electronic oscillator Zhong Ge roads signal quality is higher, and the microwave signal precision of output is also higher.
In other specific embodiments of the present utility model, the fiber unit 120 can also be dispersion shifted optical fiber Or the highly nonlinear optical fiber that length is 5km, the photodetector unit 160 can also be balanced detector.
The optical-electronic oscillator 1000 based on stimulated Brillouin scattering enlarge-effect that the present embodiment provides, believes using when multifrequency When a certain frequency in number is equal to backwards to the frequency of brillouin scattering signal, multiple-frequency signal will produce enlarge-effect, with reference to phase Position modulator 140 can produce multiple-frequency signal and the low noise feature of optical-electronic oscillator, by adjusting first laser device 100 Output wavelength changes the wavelength of brillouin scattering signal in optical fiber, so can selectivity amplification from phase-modulator 140 A certain frequency signal in the multiple-frequency signal of output, finally obtain tunable microwave signal output.The optical-electronic oscillator is not only High-precision microwave signal can be produced, and the microwave signal with wide tunable can be obtained, it greatly reduces electromagnetism and done Disturb, there is the advantages of small volume, precision are high, cost is cheap and simple in construction.
In summary, the optical-electronic oscillator provided by the utility model based on stimulated Brillouin scattering enlarge-effect utilizes cloth In deep scattered signal can amplify with its frequency identical signal characteristic, can produce multiple-frequency signal and light with reference to phase-modulator The low noise feature of electrical oscillator, by setting first laser device and second laser, make what is exported by the second laser Laser is through multiple-frequency signal caused by the phase-modulator, with the laser signal that is exported by the first laser device in fiber unit In caused by backwards to brillouin scattering signal stimulated Brillouin scattering amplification occurs, the multiple-frequency signal after amplification further passes through Overdamping, opto-electronic conversion and filtering, then two paths of signals is divided into by coupler, wherein signal is as feedback signal input phase all the way Modulator, another way signal export as microwave signal.By setting feedback circuit so that only need to adjust the defeated of first laser device Go out wavelength, you can change the frequency backwards to brillouin scattering signal, and then change in multiple-frequency signal with believing backwards to Brillouin scattering Number occur the signal frequency of stimulated Brillouin scattering amplification, then feedback signal after feedback circuit is amplified and input phase Position modulator, change the frequency distribution of the multiple-frequency signal of phase-modulator output, thus can selectivity amplification from phase A certain frequency signal in the multiple-frequency signal of modulator output, finally obtain tunable microwave signal output.Therefore, this practicality The optical-electronic oscillator of new offer can not only produce High-precision Microwave signal, and can obtain the microwave letter with wide tunable Number, and phase-modulation is carried out by feedback circuit, the external equipment of costliness is eliminated, simplifies the structure of optical-electronic oscillator, contracting Small volume, saves cost, greatly reduces electromagnetic interference, make the acquisition of adjustable microwave signal become more simple.With The upper only preferred embodiment of the present utility model, is not limited to the utility model, for the technology of this area For personnel, the utility model can have various modifications and variations.It is all within the spirit and principles of the utility model, made Any modification, equivalent substitution and improvements etc., should be included within the scope of protection of the utility model.

Claims (10)

1. a kind of optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect, it is characterised in that including first laser device, ring Shape device, fiber unit, second laser, phase-modulator, tunable attenuator, photodetector unit, tunable filter, coupling Clutch and electric amplifier;
Enter the fiber unit by the circulator from the light beam of first laser device output, and in the fiber unit It is middle to produce backwards to brillouin scattering signal;
Multiple-frequency signal is formed by the phase modulator modulation enter the optical fiber from the light beam of second laser output Unit, in the multiple-frequency signal with it is described backwards to brillouin scattering signal frequency identical signal in the fiber unit and institute State and occur to be exaggerated backwards to Brillouin scattering enlarge-effect, its power backwards to brillouin scattering signal;
Exaggerated multiple-frequency signal enters the tunable attenuator by the circulator, decays through the tunable attenuator Multiple-frequency signal afterwards is converted to electric signal through the photodetector unit;
The electric signal filters by the tunable filter, then is divided into two paths of signals by the coupler, wherein believing all the way Number enter the phase-modulator by electric amplifier amplification as feedback signal, another way signal is defeated as microwave signal Go out.
2. the optical-electronic oscillator according to claim 1 based on stimulated Brillouin scattering enlarge-effect, it is characterised in that institute First laser device is stated as wavelength and the tunable laser of power.
3. the optical-electronic oscillator according to claim 1 based on stimulated Brillouin scattering enlarge-effect, it is characterised in that institute Second laser is stated as wavelength and the tunable narrow linewidth laser of power.
4. the optical-electronic oscillator according to claim 1 based on stimulated Brillouin scattering enlarge-effect, it is characterised in that institute State the narrow linewidth laser that second laser is fixed wave length.
5. the optical-electronic oscillator according to claim 1 based on stimulated Brillouin scattering enlarge-effect, it is characterised in that institute It is single-mode fiber to state fiber unit.
6. the optical-electronic oscillator according to claim 5 based on stimulated Brillouin scattering enlarge-effect, it is characterised in that institute It is dispersion shifted optical fiber to state fiber unit.
7. the optical-electronic oscillator according to claim 5 based on stimulated Brillouin scattering enlarge-effect, it is characterised in that institute It is highly nonlinear optical fiber to state fiber unit.
8. the optical-electronic oscillator according to claim 7 based on stimulated Brillouin scattering enlarge-effect, it is characterised in that institute It is the highly nonlinear optical fiber that length is 5km to state fiber unit.
9. the optical-electronic oscillator according to claim 1 based on stimulated Brillouin scattering enlarge-effect, it is characterised in that institute It is photodetector to state photodetector unit.
10. the optical-electronic oscillator according to claim 1 based on stimulated Brillouin scattering enlarge-effect, it is characterised in that The photodetector unit is balanced detector.
CN201720152650.7U 2017-02-20 2017-02-20 Optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect Expired - Fee Related CN206673311U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201720152650.7U CN206673311U (en) 2017-02-20 2017-02-20 Optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201720152650.7U CN206673311U (en) 2017-02-20 2017-02-20 Optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect

Publications (1)

Publication Number Publication Date
CN206673311U true CN206673311U (en) 2017-11-24

Family

ID=60378687

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201720152650.7U Expired - Fee Related CN206673311U (en) 2017-02-20 2017-02-20 Optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect

Country Status (1)

Country Link
CN (1) CN206673311U (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106785812A (en) * 2017-02-20 2017-05-31 盐城工学院 Optical-electronic oscillator and adjusting method based on stimulated Brillouin scattering enlarge-effect
CN108957147A (en) * 2018-08-29 2018-12-07 中国科学院半导体研究所 Infant laser signal detection and method based on the adjustable optical-electronic oscillator of stimulated Brillouin scattering
CN110081974A (en) * 2019-05-22 2019-08-02 中国科学院长春光学精密机械与物理研究所 A kind of laser linewidth measuring system

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106785812A (en) * 2017-02-20 2017-05-31 盐城工学院 Optical-electronic oscillator and adjusting method based on stimulated Brillouin scattering enlarge-effect
CN106785812B (en) * 2017-02-20 2023-11-03 盐城工学院 Photoelectric oscillator based on stimulated Brillouin scattering amplification effect and adjusting method
CN108957147A (en) * 2018-08-29 2018-12-07 中国科学院半导体研究所 Infant laser signal detection and method based on the adjustable optical-electronic oscillator of stimulated Brillouin scattering
CN110081974A (en) * 2019-05-22 2019-08-02 中国科学院长春光学精密机械与物理研究所 A kind of laser linewidth measuring system

Similar Documents

Publication Publication Date Title
Liu et al. Integrated microwave photonic filters
Shao et al. Integrated microwave acousto-optic frequency shifter on thin-film lithium niobate
US6178036B1 (en) Opto-electronic devices and systems based on brillouin selective sideband amplification
Morrison et al. Tunable microwave photonic notch filter using on-chip stimulated Brillouin scattering
Chan et al. Microwave photonic downconversion using phase modulators in a Sagnac loop interferometer
US6766070B2 (en) High power fiber optic modulator system and method
US8014676B2 (en) CMOS-compatible tunable microwave photonic band-stop filter
CN106785812A (en) Optical-electronic oscillator and adjusting method based on stimulated Brillouin scattering enlarge-effect
CN103278941B (en) Based on microwave photon filter and the filtering method thereof of stimulated Brillouin scattering dynamic raster
Feng et al. Sharp tunable and additional noise-free optical filter based on Brillouin losses
Chew et al. Silicon-on-insulator dual-ring notch filter for optical sideband suppression and spectral characterization
CN110571627B (en) Passive compensation mode-based photoelectric oscillator with stable frequency and method thereof
Yu et al. Switchable microwave photonic filter between high Q bandpass filter and notch filter with flat passband based on phase modulation
US20080199124A1 (en) OPTICAL DEVICE FOR GENERATING AND MODULATING THz AND OTHER HIGH FREQUENCY SIGNALS
Dong Travelling-wave Mach-Zehnder modulators functioning as optical isolators
CN206673311U (en) Optical-electronic oscillator based on stimulated Brillouin scattering enlarge-effect
CN111048969B (en) Frequency doubling photoelectric oscillator based on stimulated Brillouin scattering effect
Zhu et al. Highly sensitive, broadband microwave frequency identification using a chip-based Brillouin optoelectronic oscillator
CN104113378A (en) Apparatus and method capable of tuning microwave signal source of semiconductor optical amplifier
CN108919522B (en) Ultra-narrow single-passband microwave photonic filter
Chiba et al. RF frequency sextupling via an optical two-tone signal generated from two modulation lightwaves from one Mach-Zehnder optical modulator
Chan et al. High-resolution tunable RF/microwave photonic notch filter with low-noise performance
CN109638621A (en) KHz magnitude single-pass band microwave photon filter
Zhou et al. Radio-over-fiber system with octuple frequency optical millimeter-wave signal generation using dual-parallel Mach–Zehnder modulator based on four-wave mixing in semiconductor optical amplifier
Kumar et al. Polarization controlled dispersion tunable optoelectronic oscillator and frequency octupling without bandpass filter

Legal Events

Date Code Title Description
GR01 Patent grant
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20171124