CN201263040Y - Multi-wavelength and multipath single wavelength laser based on AWG and optical fiber grating - Google Patents

Multi-wavelength and multipath single wavelength laser based on AWG and optical fiber grating Download PDF

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Publication number
CN201263040Y
CN201263040Y CNU2008201084790U CN200820108479U CN201263040Y CN 201263040 Y CN201263040 Y CN 201263040Y CN U2008201084790 U CNU2008201084790 U CN U2008201084790U CN 200820108479 U CN200820108479 U CN 200820108479U CN 201263040 Y CN201263040 Y CN 201263040Y
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fiber grating
awg
optical fiber
wavelength
fiber
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CNU2008201084790U
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Inventor
裴丽
宁提纲
董小伟
祁春慧
赵瑞峰
阮乂
延凤平
谭中伟
刘艳
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Beijing Jiaotong University
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Beijing Jiaotong University
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Abstract

The utility model relates to the fields of microwave photonics and optical fiber communication and discloses a multi-wavelength and multipath single-wavelength laser based on AWG and optical fiber gratings. Each end of 1 multiplied by N AWG (60) is connected with doped active optical fibers (20-2N), optical fiber gratings (10-1N) and WDMs (30-3N) in sequence. Pump lights (40-4N) are coupled with a branch end to the doped active optical fibers (20-2N) through WDMs (30-3N) from the one character end of AWG (60). N separate resonant cavities are formed by optical fiber gratings (11-1N) at the branch end and the optical fiber grating 10 at the one character end. The optical fiber grating (10) at the one character end is a sampling optical fiber grating or cascaded with a plurality of optical fiber gratings or wide broadband optical fiber gratings. N optical fiber gratings (11-1N) at the branch end are ordinary or polarization maintaining optical fibre gratings. Laser with N wavelengths is output from the one character end (50) and/or N-path single-wavelength laser is output from the branch ends (51-5N).

Description

Multi-wavelength and multichannel single wavelength laser based on AWG and fiber grating
Technical field
The present invention relates to optical fiber communication, microwave photon, Fibre Optical Sensor and fiber laser technology field, is a kind of multi-wavelength and multichannel single wavelength laser based on AWG and fiber grating specifically.
Background technology
Fiber-grating laser is a kind of up-and-coming light source in the optical fiber telecommunications system, its advantage is mainly reflected in: the wavelength of (1) semiconductor laser difficulty meets wavelength division multiplexing (WDM) standard of wavelength that International Telecommunications Union (ITU-T) advises, and cost is very high, and the rare-earth doped optical fibre grating laser utilizes the wavelength selectivity of fiber grating etc. can determine wavelength very exactly, and cost is very low.(2) as the rare-earth doped optical fibre manufacture craft comparative maturity of gain, rare earth ion doped process is simple, and fibre loss is little.(3) adopt the high pumping of dexterous compact efficient to become possibility.(4) fiber-grating laser has the waveguide type optical fiber structure, can produce higher power density at fiber core layer.Optical fiber structure has higher area-volume ratio, thereby radiating effect is better.Compatible good with standard traffic optical fiber can be adopted multiple fiber optic components such as fiber grating, coupler, reduces the demand of block optical element and the trouble of light path mechanical adjustment, greatly simplifies the design and the making of fiber-grating laser.(5) broadband is one of main development trend of optical fiber communication, and fiber-grating laser can be realized laser output by mixing different rare earth ions in the broadband range of 380~3900nm, and it is easy and tunable that wavelength is selected.(6) little, the anti-electromagnetic interference of the frequency chirp effect under the high frequency modulated, temperature expansion coefficient are little etc. than semiconductor laser.
Summary of the invention
Purpose of the present invention just is based on the multi-wavelength and the multichannel single wavelength laser of AWG and fiber grating, and it can overcome the deficiency of existing multi-wavelength optical fiber grating laser, realizes the stable practical multi-wavelength and the fiber laser of multi-path laser output.
The present invention proposes a kind of multi-wavelength and multichannel single wavelength laser based on AWG and fiber grating, comprising: the Waveguide array optical fiber (AWG) of a 1 * N, fiber grating are sampling optical-fiber grating or cascade fiber grating or band optical fiber grating, a N polarization-maintaining fiber grating or ordinary optic fibre grating, long doping Active Optical Fiber, a N+1 wavelength division multiplexer (WDM), the N+1 pump light of N+1 section 0.5~30m; Connection between them:
Connect one section doping Active Optical Fiber, sampling optical-fiber grating or cascade fiber grating or band optical fiber grating, WDM successively at the word end of AWG;
Divergent ends at AWG connects N section doping Active Optical Fiber, a N polarization-maintaining fiber grating or ordinary optic fibre grating, a N WDM successively;
Pump light is coupled in the doping Active Optical Fiber, and the fiber grating of divergent ends constitutes N independently resonant cavity with the fiber grating of the word end of AWG respectively, produces laser; N 〉=1.
The doping Active Optical Fiber is er-doped, mix ytterbium, mix holmium, thorium is mixed, mixed to the ytterbium erbium altogether, mix praseodymium or neodymium-doped fiber.
Beneficial effect of the present invention is specific as follows:
The doping Active Optical Fiber that existing dual wavelength fibre laser needs is inclined to one side for protecting, coupler also will be protected inclined to one side, and add the output that Polarization Detection guarantees dual wavelength single polarization fiber laser, perhaps need under low temperature such as liquid nitrogen, eliminate mode competition, produce dual wavelength; Generation to multi-wavelength is difficult more, and reliability is low, the cost height, and control is complicated, is difficult to practicality.
And the present invention adopts than protecting the much lower common Active Optical Fiber of inclined to one side Active Optical Fiber price as gain media, only needs polarization-maintaining fiber grating or/and the ordinary optic fibre grating guarantees that each laserresonator is independently.Because each laserresonator is independently, can eliminate conventional active ordinary optic fibre and produce the problem of the mode competition of dual wavelength, the stochastic model coupling can not appear.The present invention also can adopt Polarization Control to control polarization state, can obtain better laser quality.Because an end of fiber laser resonant cavity adopts sampling optical-fiber grating or cascade fiber grating or band optical fiber grating, make it easier to quasi-resonance with the reflection peak of resonant cavity other end fiber grating, reduced requirement to grating, than the easier realization of common multiple-wavelength laser, export multiwavelength laser more stable, that have higher cost performance.The parts that the present invention adopts can for protect inclined to one side or part inclined to one side for protecting, the present invention also has little, compact conformation affected by environment, characteristics such as easy to implement.
Description of drawings
Fig. 1 is that respectively there is one section doping Active Optical Fiber the both sides of AWG based on the multi-wavelength of AWG and fiber grating and multichannel single wavelength laser schematic diagram, and is two directional pump.
Fig. 2 is based on the multi-wavelength of AWG and fiber grating and multichannel single wavelength laser schematic diagram, and divergent ends one side of AWG has one section doping Active Optical Fiber, and in the unidirectional pumping of the divergent ends of AWG.
Fig. 3 is based on the multi-wavelength of AWG and fiber grating and multichannel single wavelength laser schematic diagram, and the word end of AWG has one section doping Active Optical Fiber, in the unidirectional pumping of a word end of AWG.
Among the figure: fiber grating 10, fiber grating 11-1N, doping Active Optical Fiber 20-2N, WDM30-3N, pump light 40-4N, AWG one word end 50, AWG divergent ends 51-5N, AWG60.
Embodiment
Below in conjunction with accompanying drawing multi-wavelength and multichannel single wavelength laser based on AWG and fiber grating are further described.
Embodiment one
As Fig. 1, based on the multi-wavelength and the multichannel single wavelength laser of AWG and fiber grating, the connection between the device of its formation:
Select the AWG 60 of a 1 * N, N=16.
Select the doping Active Optical Fiber 20 of 0.5m and the doping Active Optical Fiber 21~216 of 1.0m, doping Active Optical Fiber 20~216 is an Er-doped fiber.
Fiber grating 10 is selected sampling optical-fiber grating.Fiber grating 11~116 is selected the ordinary optic fibre grating.
Word end at AWG 60 connects doping Active Optical Fiber 20, fiber grating 10, WDM 30 successively.
Divergent ends at AWG 60 connects doping Active Optical Fiber 21~216, fiber grating 11~116, WDM31~316 successively.
Pump light 40~416 is coupled in the doping Active Optical Fiber 20~216 by WDM 30~316, and the fiber grating 11~116 of divergent ends constitutes 16 independently resonant cavitys with the fiber grating 10 of a word end respectively, produces laser.
16 independently the laser that produces of resonant cavity at AWG 60 1 word ends 16 wavelength lasers of 50 outputs or/and at divergent ends 51~516 outputs 16 tunnel single wavelength lasers.
Embodiment two
As Fig. 2, based on the multi-wavelength and the multichannel single wavelength laser of AWG and fiber grating, the connection between the device of its formation:
Select the AWG 60 of a 1 * N, N=32.
Select the doping Active Optical Fiber 21~232 of 1.5m, doping Active Optical Fiber 21~232 is a Yb dosed optical fiber.
Fiber grating 10 is selected cascade fiber grating.Fiber grating 11~132 is selected polarization-maintaining fiber grating.
Word end at AWG 60 connects fiber grating 10.
Divergent ends at AWG 60 connects doping Active Optical Fiber 21~232, fiber grating 11~132, WDM31~332 successively.
Pump light 41~432 is coupled in the doping Active Optical Fiber 21~232 by WDM 31~332 respectively, and the fiber grating 11~132 of divergent ends constitutes 32 independently resonant cavitys with the fiber grating 10 of a word end respectively, produces laser.
32 independently the laser that produces of resonant cavity at AWG 60 1 word ends 32 wavelength lasers of 50 outputs or/and at divergent ends 51~532 outputs 32 tunnel single wavelength lasers.
Embodiment three
As Fig. 3, based on the multi-wavelength and the multichannel single wavelength laser of AWG and fiber grating, the connection between the device of its formation:
Select the AWG 60 of a 1 * N, N=1000.
Select the doping Active Optical Fiber 20 of 15m, doping Active Optical Fiber 20 is for mixing holmium optical fiber.
Fiber grating 10 is the band optical fiber grating.Fiber grating 11~11000 is the ordinary optic fibre grating.
Word end at AWG 60 connects doping Active Optical Fiber 20, fiber grating 10, WDM30 successively.
Divergent ends at AWG 60 connects fiber grating 11~11000 respectively.
Pump light 40 is coupled in the doping Active Optical Fiber 20 by WDM 30, and the fiber grating 11~11000 of divergent ends constitutes 1000 independently resonant cavitys with the fiber grating 10 of a word end respectively, produces laser.
1000 independently the laser that produces of resonant cavity at AWG 60 1 word ends 1000 wavelength lasers of 50 outputs or/and at divergent ends 51~51000 outputs 1000 tunnel single wavelength lasers.
Embodiment four
As Fig. 1, based on the multi-wavelength and the multichannel single wavelength laser of AWG and fiber grating, the connection between the device of its formation:
Select the AWG 60 of a 1 * N.
Select the doping Active Optical Fiber 20 of one section suitable length and the doping Active Optical Fiber 21~2N of suitable length, doping Active Optical Fiber 20~2N can be for er-doped, mix ytterbium, mix holmium, thorium is mixed, mixed to the ytterbium erbium altogether, mix praseodymium or neodymium-doped fiber.
Fiber grating 10 is sampling optical-fiber grating or cascade fiber grating or band optical fiber grating.Fiber grating 11-1N is polarization-maintaining fiber grating or ordinary optic fibre grating.
Word end at AWG 60 connects doping Active Optical Fiber 20, fiber grating 10, WDM 30 successively.
Divergent ends at AWG 60 connects doping Active Optical Fiber 21~2N, fiber grating 11~1N, WDM31~3N successively.
Pump light 40~4N is coupled among doping Active Optical Fiber 20~2N by WDM30~3N, and the fiber grating 11~1N of divergent ends constitutes N independently resonant cavitys with the fiber grating 10 of a word end respectively, produces laser.
The laser that the individual independently resonant cavity of N produces is exported N wavelength lasers or/and at the single wavelength laser in divergent ends 51~5N output N road at AWG 60 1 word ends 50.

Claims (4)

1. based on the multi-wavelength and the multichannel single wavelength laser of AWG and fiber grating, it is characterized in that this laser comprises: the AWG of a 1 * N (60), fiber grating (10-1N), doping Active Optical Fiber (20-2N), WDM (30-3N), pump light (40-4N); Connection between them:
Select the long doping Active Optical Fiber (20~2N) of 0.5~30m;
Fiber grating (10) is sampling optical-fiber grating or cascade fiber grating or band optical fiber grating, and fiber grating (11-1N) is polarization-maintaining fiber grating or ordinary optic fibre grating;
Word end at AWG (60) connects doping Active Optical Fiber (20), fiber grating (10), WDM (30) successively;
The divergent ends of AWG (60) connect successively the doping Active Optical Fiber (21~2N), fiber grating (11~1N), WDM (31~3N);
Pump light (40~4N) by WDM (30~3N) are coupled into the doping Active Optical Fiber, and (in 20~2N), (11~1N) constitute N independently resonant cavity with the fiber grating (10) of the word end of AWG (60) respectively to the fiber grating of divergent ends, produce laser; N 〉=1.
2. multi-wavelength and multichannel single wavelength laser based on AWG and fiber grating according to claim 1 is characterized in that, the doping Active Optical Fiber (20~2N) for er-doped, mix ytterbium, mix holmium, thorium is mixed, mixed to the ytterbium erbium altogether, mix praseodymium or neodymium-doped Active Optical Fiber.
3. multi-wavelength and multichannel single wavelength laser based on AWG and fiber grating according to claim 1, it is characterized in that, word end at AWG (60) connects fiber grating (10), (41~4N) (31~3N) are coupled into the doping Active Optical Fiber (in 21~2N) to pump light by WDM respectively, (11~1N) constitute N independently resonant cavity with the fiber grating (10) of AWG (60) one word ends respectively to the fiber grating of divergent ends, at N wavelength laser of AWG (60) one word ends (50) output or/and at divergent ends (51~5N) output N roads list wavelength lasers.
4. multi-wavelength and multichannel single wavelength laser based on AWG and fiber grating according to claim 1, it is characterized in that, divergent ends at AWG (60) connects fiber grating (11~1N), pump light (40) is coupled in the doping Active Optical Fiber (20) by WDM (30), (11~1N) constitute N independently resonant cavity with the fiber grating (10) of AWG (60) one word ends respectively to the fiber grating of divergent ends, at N wavelength laser of AWG (60) one word ends (50) output or/and at divergent ends (51~5N) output N roads list wavelength lasers.
CNU2008201084790U 2008-06-06 2008-06-06 Multi-wavelength and multipath single wavelength laser based on AWG and optical fiber grating Expired - Fee Related CN201263040Y (en)

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102570255A (en) * 2011-12-30 2012-07-11 北京交通大学 Multi-wavelength optical fiber laser
CN110137797A (en) * 2019-05-10 2019-08-16 上海电力学院 A method of generating ultrahigh frequency pulses

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102570255A (en) * 2011-12-30 2012-07-11 北京交通大学 Multi-wavelength optical fiber laser
CN110137797A (en) * 2019-05-10 2019-08-16 上海电力学院 A method of generating ultrahigh frequency pulses
CN110137797B (en) * 2019-05-10 2020-10-09 上海电力学院 Method for generating ultrahigh frequency pulse

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