CN102508388A - Optical fiber parameter amplifier - Google Patents
Optical fiber parameter amplifier Download PDFInfo
- Publication number
- CN102508388A CN102508388A CN2011103654386A CN201110365438A CN102508388A CN 102508388 A CN102508388 A CN 102508388A CN 2011103654386 A CN2011103654386 A CN 2011103654386A CN 201110365438 A CN201110365438 A CN 201110365438A CN 102508388 A CN102508388 A CN 102508388A
- Authority
- CN
- China
- Prior art keywords
- optical fiber
- magnetic field
- adjustable
- unit
- magneto
- 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.)
- Pending
Links
Images
Landscapes
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
The invention discloses an optical fiber parameter amplifier. The optical fiber parameter amplifier comprises an input coupling unit, a pump light source unit, a magnetically-adjustable non-linear optical fiber unit and a light filter output unit, and is characterized in that the magnetically-adjustable non-linear optical fiber unit comprises a magneto-optical non-linear optical fiber, a magnetic field applying device and an adjustable direct current power supply, wherein the adjustable direct current power supply supplies adjustable current to the magnetic field applying device, and the magnetic field applying device supplies a magnetic field to the magneto-optical non-linear optical fiber. The optical fiber parameter amplifier supplies a driving current to the magnetic field applying device through the adjustable direct current power supply to adjust the magnetic field applied to the magneto-optical non-linear optical fiber, so as to realize an electromagnetic adjustment process and control parameter gains, avoid the deterioration of the performance of the optical fiber parameter amplifier caused by the conventional gain adjusting way, further improve the gain performance of the optical fiber parameter amplifier, and meet the requirement on a relatively long relay distance.
Description
Technical field
The invention belongs to technical field of optical fiber communication, be specifically related to a kind of design of optical fiber parameter amplifier.
Background technology
Along with developing rapidly of Networks of Fiber Communications; Optical communication system is more and more urgent to the optical information processing technology requirement, for example requires image intensifer to have big gain bandwidth (GB), high-gain level and saturation output power, low-noise factor and multiple signals while amplifying power etc.Optical Amplification Technology is the focus of optical communication field research having huge advantage and potentiality aspect optical communication system dilatation and the increase transmission range always.Traditional Erbium-Doped Fiber Amplifier (EDFA) has been difficult to adapt to the development of following optical-fiber network to a certain extent at aspects such as gain bandwidth (GB), noiseproof features.
Optical fiber parameter amplifier (FOPA, Fiber Optical Parametric Amplifier) based on optical fiber four-wave mixing (FWM, Four-Wave Mixing) nonlinear effect more and more receives publicity, and becomes the focus of research.Optical fiber parameter amplifier is to rely on the four-wave mixing effect in the optical fiber to carry out the new type light amplifier that light signal amplifies; Image intensifer contrast with other type; Optical fiber parameter amplifier has many remarkable advantages: high-gain (when small-signal is similar to, with the pump power exponent function relation), wide bandwidth (can all band work in optical communication system), phase-sensitive nature (can realize that the 0dB spontaneous emission noise amplifies), multiple signals are amplifying power and low noise figure etc. simultaneously.
In order to adapt to the requirement of long repeater span in the optical fiber communication, perhaps make relevant optical fiber information processing device such as Fiber-optic parametric oscillator etc. be operated in suitable duty, often need control the gain of optical fiber parameter amplifier.The gain of optical fiber parameter amplifier is relevant with pump power, so can adopt traditional adjusting pump power mode to control the size of optical fiber parameter amplifier signal gain.Though size that can the adjustable parameter gain in this traditional Gain Adjustable mode ordinary optic fibre that useful area is bigger in that nonlinear factor is less; But the gain that is obtained can not be satisfied the requirement of long repeater span; This just need increase a plurality of repeaters between both communications; Thereby increased the expense of equipment; And pump power affects the phase mismatch of four-wave mixing, when the certain limit pump power, can make phase place can not reach matching condition four-wave mixing efficient is reduced, thus the dynamic property that this adjustable mode can the deterioration signal gain.
Summary of the invention
The objective of the invention is to have proposed a kind of optical fiber parameter amplifier in order to solve the problems referred to above that existing optical fiber parameter amplifier exists.
Technical scheme of the present invention is: a kind of optical fiber parameter amplifier; Comprise: input coupling unit, pump light source unit, magnetic is adjustable nonlinear optical fiber unit and optical filter output unit; Pump light that said pump light source unit sends and input signal light obtain ideler frequency light and flashlight through input coupling unit and the adjustable nonlinear optical fiber of magnetic unit successively; After optical filter output unit output signal output; It is characterized in that described magnetic is adjustable, and the nonlinear optical fiber unit comprises magneto-optic nonlinear optical fiber, magnetic field charger and adjustable direct supply, wherein; Adjustable direct supply provides adjustable electric current for the magnetic field charger, and the magnetic field charger provides magnetic field for the magneto-optic nonlinear optical fiber.
Further, described magnetic field charger is a helical ring type magnetic field charger, perhaps is solenoid type magnetic field charger.
Beneficial effect of the present invention: under the same conditions, optical fiber parameter amplifier of the present invention can further improve the size of parametric gain on the basis of traditional adjusting pump power mode; Optical fiber parameter amplifier of the present invention has electromagnetism regulative mode advantage, promptly for the magnetic field charger drive current is provided through adjustable direct supply, is applied to the magnetic field on the magneto-optic nonlinear optical fiber with adjusting, thereby realizes the electromagnetism adjustment process, the control parametric gain.
The present invention adopts the magneto-optic nonlinear optical fiber as parameter media implementation gain enlarging function; And realize the adjustable function of parametric gain through electromagnetic mode; Not only overcome the deterioration of traditional gain-adjusted mode to the optical fiber parameter amplifier performance; But also can further promote the gain performance of traditional fiber parameter amplifier; Make its requirement of satisfying longer repeater span, and can also carry out shaping feature to the output pulse, can be applied in fields such as optical fiber communication and intelligent optical information processing through this regulative mode.
Description of drawings
Fig. 1 is the principle schematic of optical fiber parameter amplifier gain control of the present invention.
Fig. 2 is the synoptic diagram of pump light source of the present invention unit.
Fig. 3 is the adjustable nonlinear optical fiber cell schematics of magnetic of the present invention.
Fig. 4 is a helical ring type magnetic field charger synoptic diagram in the adjustable nonlinear optical fiber of the magnetic of the present invention unit.
Fig. 5 is a solenoid type magnetic field charger synoptic diagram in the adjustable nonlinear optical fiber of the magnetic of the present invention unit.
Fig. 6 is that optical fiber parameter amplifier signal gain of the present invention is with the periodically variable synoptic diagram of fiber lengths.
Fig. 7 is fiber lengths of the present invention optical fiber parameter amplifier signal gain adjustable extent synoptic diagram when being 100m.
Embodiment
Below in conjunction with accompanying drawing and concrete embodiment the present invention is done further elaboration.
The optical fiber parameter amplifier that the present invention proposes comprises input coupling unit, pump light source unit, magnetic is adjustable nonlinear optical fiber unit, optical filter output unit.The present invention is based on magneto-optic effect and the interactional new mechanism of four-wave mixing, regulates both couplings through the magnetic control mode.Four-wave mixing effect takes place in the flashlight and the pump light of coupling in the adjustable nonlinear optical fiber of magnetic unit; And magneto-optic effect will change in the magneto-optic nonlinear optical fiber under the effect of regulating externally-applied magnetic field; And then affecting the oval birefringence in the magneto-optic nonlinear optical fiber, oval birefringence can be regarded as the magnetic circular birefringence that caused by magneto-optic effect and the stack of linear birefringence.Because four-wave mixing efficient is relevant with the guided wave polarization state of light; And oval birefringent change affects the polarization state that guided wave transmits in the magneto-optic nonlinear optical fiber in the magneto-optic nonlinear optical fiber; The conversion of this polarization state is caused by magneto-optic effect, and available magneto-optic coupling coefficient κ
mMeasure magneto-optic coupling coefficient κ
mEqual Verdet constant V
BWith the product of magnetic induction density B, i.e. κ
m=V
BB.So realize the magnetic controllable device through externally-applied magnetic field, the oval birefringence of the magneto-optic nonlinear optical fiber of system is changed, thus signal gain in the control Fiber-optic parametric process.Magneto-optic optical fiber based on this magneto-optic effect and nonlinear fiber has been applied in Fibre Optical Sensor, grating and the magneto-optic shutter etc.; Also realized simultaneously the magneto-optic nonlinear optical information processing function; Can be used for the squeezed light pulse like magneto-optic effect with from the frequency chirp that the coupling of phase modulation (PM) (SPM) or cross-phase modulation (XPM) produces, and cross-phase modulation (XPM) magneto-optic shutter etc.
Situation during with respect to no externally-applied magnetic field changes the adjustable extent that is defined as parametric gain with the peak signal gain that can obtain under the magnetic control condition.
Be that the single channel optical fiber parameter amplifier of 9dB is an example with the parametric gain adjustable extent below, specify.
Optical fiber parameter amplifier as shown in Figure 1 comprises input coupling unit, pump light source unit, magnetic is adjustable nonlinear optical fiber unit, optical filter output unit.Pump light that the pump light source unit sends and input signal light are input to the adjustable nonlinear optical fiber of magnetic unit through the input coupling unit; The efficient of in the adjustable nonlinear optical fiber of magnetic unit, regulating four-wave mixing through the adjustability of magneto-optic effect; After optical filter output unit output signal output is realized separating of flashlight and ideler frequency light.
Here, the input coupling unit comprises Polarization Controller (PC, Polarization Controller) and coupling mechanism, and the Polarization Controller effect is to make input signal light and pump light convert required polarization state into.
Here; The function of optical filter output unit is to realize separating of flashlight and ideler frequency light; At this for single channel optical fiber parameter amplifier as shown in Figure 1; Owing to will be two bundle flashlight and ideler frequency light,, then the ideler frequency light blocking be made flashlight output so the optical filter output unit can be optical band pass filter through the light of optical filter output unit; For the multichannel optical fiber parameter amplifier, the optical filter output unit also can be optical band pass filter or comb filter.
Here, the pump light source unit is as shown in Figure 2, specifically comprises pump laser and image intensifer, perhaps adopts other high power laser light source; When output pumping power ratio is big; Said pump light source unit also comprises stimulated Brillouin scattering (SBS; Stimulated Brillouin Scattering) suppresses module; Stimulated Brillouin scattering suppresses module and mainly comprises phase-modulator, cosine wave signal generator etc., and the pump light of its output produces after phase modulation (PM).Owing in optical fiber, there is the stimulated Brillouin scattering effect; When input pumping light power during greater than the stimulated Brillouin scattering threshold value; The stimulated Brillouin scattering effect can produce back scattering; Influence parametric gain thereby pumping light power is descended, phase modulation (PM) then is to improve the method for stimulated Brillouin scattering threshold value.
Here; Magnetic is adjustable, and the nonlinear optical fiber unit is as shown in Figure 3, specifically comprises magneto-optic nonlinear optical fiber, magnetic field charger, adjustable direct supply, wherein; Adjustable direct supply provides adjustable electric current for the magnetic field charger, and the magnetic field charger provides magnetic field for the magneto-optic nonlinear optical fiber.Here adopt the magneto-optic nonlinear optical fiber as the parameter medium, under suitable accurate phase matching or complete matching condition, realize magneto-optic four-wave mixing parametric gain amplification.Influence of magnetic field through the magnetic field charger produces the evolution distribution of guided wave polarization state in magneto-optic optical fiber, and then affects the purpose that four-wave mixing efficient reaches the gain of control Fiber-optic parametric.Can regulate the size of electric current according to adjustable direct supply; Realize the adjustability of magneto-optic effect in the charger of magnetic field; In order to the guided wave light-transfer characteristic in the control magneto-optic nonlinear optical fiber, and then the efficient of regulating four-wave mixing in the magneto-optic nonlinear optical fiber, reach the purpose that improves parametric gain.
On the one hand, produce the adjustable processing of magnetic that the magnetic field size realizes the magneto-optic nonlinear optical fiber, make magneto-optic effect different the transmission influence of guided wave in the optical fiber through changing the magnetic field charger; On the other hand, owing to also have linear birefringence in the magneto-optic nonlinear optical fiber, the magnetic circular birefringence that is caused by magneto-optic effect and the stack of linear birefringence have formed the oval birefringence in the magneto-optic nonlinear optical fiber.Therefore change the oval birefringence of magneto-optic nonlinear optical fiber through the magnetic tunable characteristic, and then affected the efficient of four-wave mixing.
Choosing of magneto-optic nonlinear optical fiber length affects parametric gain in the magnetic here the is adjustable nonlinear optical fiber unit; And then the magnetic adjustability will show different characteristic to the effect of parametric gain when different fiber length; Simultaneously as required during fixed fiber length, can show of the influence of magnetic adjustability to parametric gain.
To be that 50mw, wavelength are that pump light and the power input of 1549nm is that 1mw, wavelength are that the flashlight of 1560nm sends to the input coupling unit together by the power that the pump light source unit sends.At this moment, the pump light source unit comprises pump laser and image intensifer, perhaps adopts other high power laser light source; When output pumping power ratio was big, the pump light source unit comprised that also stimulated Brillouin scattering suppresses module, and stimulated Brillouin scattering suppresses module and mainly comprises phase-modulator, cosine wave signal generator etc., and is as shown in Figure 2.Reduce four-wave mixing efficient even the pumping light power of input can not make the phase place of four-wave mixing reach matching condition, but can be increased in signal gain in this case through magnetic adjustability of the present invention.
Pump light and flashlight convert required polarization state into through Polarization Controller in the input coupling unit, and then light wavelength division multiplexing effect co-transmitted arrives the adjustable nonlinear optical fiber of magnetic unit in the input coupling unit.
Magnetic is adjustable, and the nonlinear optical fiber unit comprises magneto-optic nonlinear optical fiber, magnetic field charger and adjustable direct supply, and is as shown in Figure 3.
To the magnetic field charger, the magnetic approach of loading is varied; It is more convenient to adopt the mode of spiral rings to add loaded magnetic field comparatively speaking, and the winding of optical fiber in spiral rings realize easily, has avoided the influence of flexibility to optical fiber property.Spiral rings produces magnetic field and can twine through single line, also can through two-wire and around mode (adopting enamel covered wire usually).
The spiral rings structure that Fig. 4 shows two-wire and realizes around mode.No matter guided wave is to propagate along magnetic direction or counter field direction in the magneto-optic nonlinear optical fiber, turning to of vibration plane is all the same, and it is determined by magnetic direction, promptly depends on coiling 1 (A1-B1) and coiling 2 (A2-B2) connected mode.When terminal B 1 links to each other with B2, when A1 and A2 are connected on the two poles of the earth of adjustable direct supply respectively, can know to cancel out each other in the magnetic field of generation in the spiral rings, can not realize adding the purpose of loaded magnetic field.Can find out through analyzing; With terminal A 2 with after B1 links to each other; A1 and B2 are connected on respectively on the two poles of the earth of adjustable direct supply, perhaps A1 and A2, B1 be connected on respectively on the two poles of the earth of adjustable direct supply after B2 links to each other; The interior magnetic direction unanimity of spiral rings this moment makes the magnetic field intensity in its spiral rings reach maximal value.Present embodiment adopts A1 and A2, realization magnetic field loading on B1 and the two poles of the earth that are connected on adjustable direct supply after B2 links to each other respectively.The direction of learning loading current as shown in Figure 4 can know that by Amp the direction of spiral rings internal magnetic field is counterclockwise.
The length of parametric gain characteristic and magneto-optic nonlinear optical fiber is closely related.Optical signal gain is along with fiber lengths periodically changes, and is as shown in Figure 6, and along with the difference of fiber lengths, the adjustable extent of parametric gain also will show different characteristic.In the adjustable nonlinear optical fiber of magnetic unit, the Verdet constant V of magneto-optic nonlinear optical fiber
BBe respectively 32rad/ (Tm) and 1W with nonlinear factor
-1/ km; The length of magneto-optic nonlinear optical fiber is taken as 100m, and it is wrapped in the torus, and is as shown in Figure 4.Provide the adjustable direct supply of drive current to change the magnetic field that is applied on the magneto-optic nonlinear optical fiber through being adjusted to the magnetic field charger; Guided wave light-transfer characteristic in the may command magneto-optic nonlinear optical fiber; And then the efficient of regulating four-wave mixing in the magneto-optic nonlinear optical fiber, reach the purpose that adjustable parameter gains.
The magnetic field charger also can adopt the magnetic field charger of solenoid type, and concrete structure is as shown in Figure 5.Produce maximum magnetic field intensity in the solenoid in order to make; Loading current direction as shown in the figure; Can know that by Amp the magnetic direction in the solenoid is from left to right, then the magnetic field charger with the helical ring type is identical to the operation of the magnetic field charger of solenoid type.
For single pass optical fiber parameter amplifier; The optical filter output unit can the selective light BPF.; The parameter amplifying signal is through optical band pass filter output, and corresponding parametric gain adjustable extent can satisfy the designing requirement of 9dB, and is as shown in Figure 7; Simultaneously can find out that the magneto-optic coupling coefficient applies magnetic field and also helps to improve signal gain when 0 to 0.2rad/m scope.
The advantage of the relative existing fiber parameter amplifier of the present invention is: (1) under the same conditions, the present invention can further improve the size of parametric gain on the basis of traditional adjusting pump power mode.(2) has electromagnetism regulative mode advantage.The present invention provides drive current through adjustable direct supply for the magnetic field charger, is applied to the magnetic field on the magneto-optic nonlinear optical fiber with adjusting, thereby realizes the electromagnetism adjustment process, the control parametric gain.(3) optical fiber parameter amplifier of the present invention has flexible and controllable and simple and easy implementation, can be applied in fields such as optical fiber communication and intelligent optical information processing.
Those of ordinary skill in the art will appreciate that embodiment described here is in order to help reader understanding's principle of the present invention, should to be understood that protection scope of the present invention is not limited to such special statement and embodiment.Those of ordinary skill in the art can make various other various concrete distortion and combinations that do not break away from essence of the present invention according to these teachings disclosed by the invention, and these distortion and combination are still in protection scope of the present invention.
Claims (4)
1. optical fiber parameter amplifier; Comprise: input coupling unit, pump light source unit, magnetic is adjustable nonlinear optical fiber unit and optical filter output unit; Pump light that said pump light source unit sends and input signal light obtain ideler frequency light and flashlight through input coupling unit and the adjustable nonlinear optical fiber of magnetic unit successively; After optical filter output unit output signal output; It is characterized in that described magnetic is adjustable, and the nonlinear optical fiber unit comprises magneto-optic nonlinear optical fiber, magnetic field charger and adjustable direct supply, wherein; Adjustable direct supply provides adjustable electric current for the magnetic field charger, and the magnetic field charger provides magnetic field for the magneto-optic nonlinear optical fiber.
2. optical fiber parameter amplifier according to claim 1 is characterized in that, described magnetic field charger is a helical ring type magnetic field charger, perhaps is solenoid type magnetic field charger.
3. optical fiber parameter amplifier according to claim 1 and 2 is characterized in that, described optical filter output unit is an optical band pass filter.
4. optical fiber parameter amplifier according to claim 1 and 2 is characterized in that, described optical filter output unit can be comb filter.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN2011103654386A CN102508388A (en) | 2011-11-17 | 2011-11-17 | Optical fiber parameter amplifier |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN2011103654386A CN102508388A (en) | 2011-11-17 | 2011-11-17 | Optical fiber parameter amplifier |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN102508388A true CN102508388A (en) | 2012-06-20 |
Family
ID=46220491
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN2011103654386A Pending CN102508388A (en) | 2011-11-17 | 2011-11-17 | Optical fiber parameter amplifier |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN102508388A (en) |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN106225816A (en) * | 2016-07-01 | 2016-12-14 | 南京大学 | A kind of grating sensing apparatus and method based on Brillouin's wave filter |
| CN112993731A (en) * | 2019-12-13 | 2021-06-18 | 华为技术有限公司 | Gain adjuster, gain adjusting method and optical line terminal |
| CN114062981A (en) * | 2021-11-04 | 2022-02-18 | 上海交通大学 | Quantum-enhanced magnetic field gradiometer and magnetometer |
| CN115112935A (en) * | 2022-06-28 | 2022-09-27 | 中国长江三峡集团有限公司 | Optical fiber terminal device and data transmission system |
| CN115642467A (en) * | 2022-12-23 | 2023-01-24 | 武汉光谷航天三江激光产业技术研究院有限公司 | Method and system for inhibiting stimulated Brillouin scattering effect of optical fiber laser |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102075249A (en) * | 2010-12-03 | 2011-05-25 | 电子科技大学 | Device for processing nonlinear information of magnet adjustable optical fiber |
| CN202362561U (en) * | 2011-11-17 | 2012-08-01 | 电子科技大学 | Optical fiber parametric amplifier |
-
2011
- 2011-11-17 CN CN2011103654386A patent/CN102508388A/en active Pending
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102075249A (en) * | 2010-12-03 | 2011-05-25 | 电子科技大学 | Device for processing nonlinear information of magnet adjustable optical fiber |
| CN202362561U (en) * | 2011-11-17 | 2012-08-01 | 电子科技大学 | Optical fiber parametric amplifier |
Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN106225816A (en) * | 2016-07-01 | 2016-12-14 | 南京大学 | A kind of grating sensing apparatus and method based on Brillouin's wave filter |
| CN106225816B (en) * | 2016-07-01 | 2018-06-08 | 南京大学 | A kind of grating sensing apparatus and method based on Brillouin's wave filter |
| CN112993731A (en) * | 2019-12-13 | 2021-06-18 | 华为技术有限公司 | Gain adjuster, gain adjusting method and optical line terminal |
| CN112993731B (en) * | 2019-12-13 | 2022-10-04 | 华为技术有限公司 | Gain adjuster, gain adjusting method and optical line terminal |
| CN114062981A (en) * | 2021-11-04 | 2022-02-18 | 上海交通大学 | Quantum-enhanced magnetic field gradiometer and magnetometer |
| CN114062981B (en) * | 2021-11-04 | 2022-11-29 | 上海交通大学 | Magnetic field gradiometer, magnetometer of quantum reinforcing |
| CN115112935A (en) * | 2022-06-28 | 2022-09-27 | 中国长江三峡集团有限公司 | Optical fiber terminal device and data transmission system |
| CN115112935B (en) * | 2022-06-28 | 2023-06-20 | 中国长江三峡集团有限公司 | Optical fiber terminal device and data transmission system |
| CN115642467A (en) * | 2022-12-23 | 2023-01-24 | 武汉光谷航天三江激光产业技术研究院有限公司 | Method and system for inhibiting stimulated Brillouin scattering effect of optical fiber laser |
| CN115642467B (en) * | 2022-12-23 | 2023-03-28 | 武汉光谷航天三江激光产业技术研究院有限公司 | Method and system for inhibiting stimulated Brillouin scattering effect of optical fiber laser |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Okuno et al. | Silica-based functional fibers with enhanced nonlinearity and their applications | |
| CN103278941B (en) | Based on microwave photon filter and the filtering method thereof of stimulated Brillouin scattering dynamic raster | |
| CN103296569A (en) | Super-continuum spectrum light source based on dual-band seed source Er-Yb co-doped optical fiber amplifier | |
| CN102508388A (en) | Optical fiber parameter amplifier | |
| CN104330939A (en) | SBS broadband tunable optical fiber delay system | |
| EP1076428B1 (en) | Optical fiber communication system employing wavelength converter for broadband transmission | |
| Wada et al. | Modal gain controllable 2-LP-mode fiber amplifier using PLC type coupler and long-period grating | |
| CN202362561U (en) | Optical fiber parametric amplifier | |
| CN102540623B (en) | Scheme and device for increasing gain of optical fiber parametric amplifier by adopting phase-shifting grating | |
| CN102075249B (en) | Device for processing nonlinear information of magnet adjustable optical fiber | |
| CN103278998A (en) | Fiber parameter amplification system for improving energy conversion efficiency of pump light to signal light | |
| Khaki et al. | Transient correction using EDFA: in-line optical fiber with feedback | |
| CN1556561A (en) | Wave length tunable narrow wire width, high signal noise ratio single polarization ring cavity full optical fiber laser | |
| CN107577102A (en) | A kind of double pumping action optical fiber parameter amplifier based on photonic crystal fiber | |
| CN202854463U (en) | Single pumping light fiber parametric amplifier capable of filtering idler frequency light and achieving gain optimization | |
| Mustafa et al. | Multi-pumped Raman amplifier for long-haul UW-WDM optical communication systems: gain flatness and bandwidth enhancements | |
| Ummy et al. | Extending the gain bandwidth of combined Raman-parametric fiber amplifiers using highly nonlinear fiber | |
| CN202334535U (en) | Bi-directional multichannel light-operated optical information processing device | |
| CN202720428U (en) | Device for improving gain of fiber parameter amplifier by adopting phase-shifting grating | |
| CN104898304A (en) | Photonic microwave filter introducing infinite impulse response | |
| CN111952828B (en) | Device for improving signal light gain by adopting twin-core and twin-pump optical fiber parametric amplifier | |
| CN204597214U (en) | A kind of mixing discrete highly nonlinear optical fiber amplifier based on two feedback arrangement | |
| CN104821481B (en) | A kind of mixing discrete highly nonlinear optical fiber amplifier based on double feedback arrangements | |
| Chan et al. | Dispersion-compensating fiber Raman amplifiers with step, parabolic, and triangular refractive index profiles | |
| CN203551923U (en) | Optical fiber parametric amplification system improving energy conversion efficiency from pump light to signal light |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C06 | Publication | ||
| PB01 | Publication | ||
| C10 | Entry into substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| C12 | Rejection of a patent application after its publication | ||
| RJ01 | Rejection of invention patent application after publication |
Application publication date: 20120620 |