CN1688069A - Phase locking multi-light beam coherent superimposed optical fiber laser - Google Patents

Phase locking multi-light beam coherent superimposed optical fiber laser Download PDF

Info

Publication number
CN1688069A
CN1688069A CN 200510016772 CN200510016772A CN1688069A CN 1688069 A CN1688069 A CN 1688069A CN 200510016772 CN200510016772 CN 200510016772 CN 200510016772 A CN200510016772 A CN 200510016772A CN 1688069 A CN1688069 A CN 1688069A
Authority
CN
China
Prior art keywords
laser
polarization
fiber
maintaining
tapered
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
CN 200510016772
Other languages
Chinese (zh)
Other versions
CN1331280C (en
Inventor
王蓟
王国政
***
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.)
Changchun Institute of Optics Fine Mechanics and Physics of CAS
Original Assignee
Changchun Institute of Optics Fine Mechanics and Physics of CAS
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 Changchun Institute of Optics Fine Mechanics and Physics of CAS filed Critical Changchun Institute of Optics Fine Mechanics and Physics of CAS
Priority to CNB2005100167725A priority Critical patent/CN1331280C/en
Publication of CN1688069A publication Critical patent/CN1688069A/en
Application granted granted Critical
Publication of CN1331280C publication Critical patent/CN1331280C/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Lasers (AREA)
  • Optical Communication System (AREA)
  • Optical Couplings Of Light Guides (AREA)

Abstract

This invention relates to a phase-locking multi-beam coherent addition fiber laser, which is made up of a fiber laser outputting polarized lights, a fiber phase modulator, a fiber amplifier, a melted tapered polarization maintaining fiber coupler and a feed-back control circuit. It is a fiber laser with high bean quality as well as outputting high power by phase-locking multi-beam coherent addition.

Description

Phase locking multi-light beam coherent superimposed optical fiber laser
Technical field:
The present invention relates to fiber laser, specifically, belong to the fiber laser of phase locking multi-laser beam coherent superposition output.
Technical background:
The length historical about the same of the history of fiber laser and laser itself.Laser came out soon, and the Znitzer of U.S. Optical Co., Ltd (American optical corporation) and Koestor have at first proposed the design of fiber laser and amplifier in 1963.Fiber laser has that efficient height, threshold value are low, line width, tunable, characteristics such as compactness is small and exquisite, the ratio of performance to price is high, be easy to make, wavelength is abundant, has purposes very widely in optical communication, industrial processes, medical science, scientific research, image record and printing, computer and fields such as microelectronics manufacturing, spectroscopy.With the multiple laser stack,, can obtain the laser of high power and nearly diffraction limit if satisfy complete coherent condition between the multiple laser.The laser identical to the N beam power carries out non-coherent addition, and then light intensity increases N doubly, and if carry out coherent superposition, then amplitude increases N doubly, light intensity increases N 2Doubly.Consider that from benefit and expense the scheme of coherent superposition is better.But want to realize the coherent superposition between the multiple laser, the condition of the phase matched that must satisfy that frequency is identical, polarization one is made peace, the phase place of conventional laser device output laser all has random drift, and every Shu Jiguang may cause producing phase difference between each Shu Jiguang through different light paths; For the polarization state of each laser beam, even the laser of exporting from light source is linear polarization, after the Optical Fiber Transmission through a segment distance, because the mode birefringence of optical fiber, polarization state also can change; Frequency for each laser beam, nonlinear effect in the optical fiber may cause between each laser beam and produce frequency difference, therefore want to realize that the relevant frequency that must control each laser beam well of multiple laser is identical, polarization one is made peace phase matched, to reach complete coherent condition.
At present, mostly the method that realizes the stack of multiple beams of optical fiber laser is by the non-coherent addition method, tie into many output optical fibres of fiber laser a branch of, can realize high-power fiber laser, but output is multimode light, beam quality factor is several mm*mrad even tens mm*mrad, and beam quality is very poor, and this has just limited this fiber laser and can only be applied to the less demanding industrial circle of beam quality.Research for the optical-fiber laser coherent superposition still is in laboratory stage, people such as S.J.Augst are to the synthetic experimental study that carried out of the fine laser coherence of two-beam, realized the fine laser coherence stack of two-beam by phase locking, but owing in structure, introduced anamorphic prism to non-fiber optic components such as, spectroscopes, do not realize the structure of full fiberize, the introducing of non-fiber optic component has also limited the getable maximum power of system, has also only realized the coherent superposition of the fine laser of two-beam.
Summary of the invention:
In order to solve the superimposed light beam energy that the multiple laser non-coherent addition exists is the simple addition of each laser beam energy, the bad problem of beam quality of stack back multimode output, the present invention has realized the phase locking to multiple laser, a kind of relevant fully back output single-mode laser is provided, obtains than superpose high power more and have the fiber laser of better beam quality simultaneously of the common multi-laser beam that does not carry out phase locking.
The present invention includes the fiber laser 1 of output polarization light, polarization maintaining optical fibre isolator 2,1 * N+1 melts tapered polarization-maintaining fiber coupler 3, fibre optic phase modulator 4, fiber amplifier 5,90: 10 polarization-maintaining fiber coupler 6,1 * N melt tapered polarization-maintaining fiber coupler 7,1 * 2 and melt tapered polarization-maintaining fiber coupler 8, feedback control circuit 9, lens 10, avalanche photodide or PIN photodiode 11, high-frequency amplifier 12.Whole system is all used polarization maintaining optical fibre, and guarantee that N bundle laser melts the equivalent optical path of the light path of tapered polarization-maintaining fiber coupler 8 by 90: 10 polarization-maintaining fiber couplers 6 to 1 * 2, guarantee that N bundle laser melts tapered polarization-maintaining fiber coupler 7 to 1 * 2 by 1 * N and melts the equivalent optical path of the light path of tapered polarization-maintaining fiber coupler 8.
The function of fiber laser 1 provides linearly polarized laser.
The function of polarization maintaining optical fibre isolator 2 is the polarized laser beam one-way transmissions that guarantee output from the fiber laser 1 of output polarization light, the harm that the reverberation that prevents from may to occur in the light path may bring fiber laser 1, and then the stability of raising system, reduce noise effect.
The function that 1 * N+1 melts tapered polarization-maintaining fiber coupler 3 is that a branch of polarization laser is divided into the N+1 bundle, keeps N+1 bundle laser polarization state identical simultaneously, in this N+1 bundle laser, beam of laser is arranged as the reference laser beam, is divided into the N bundle in secondary light path B; Other modulated in main optical path A, the amplification of N bundle polarization laser, relevant fully back laser intensity is N 2Increase, can obtain the laser output that high power has high light beam quality simultaneously.
The function of fibre optic phase modulator 4 is the phase differences between the compensation N bundle optical-fiber laser, reach desirable precise phase modulation, fibre optic phase modulator 4 receives the feedback signal that feedback control circuit 9 gives, make main optical path A go up the phase place unanimity of N bundle optical-fiber laser, realize phase locking, use fibre optic phase modulator 4 fundamentally to reduce the insertion loss and the echo reflection of device.
The function of fiber amplifier 5 is the power amplifications of N being restrainted optical-fiber laser, although after N bundle optical-fiber laser was concerned with fully, intensity was the N of single beam laser intensity 2Doubly, but want to realize high power laser light output, must carry out power amplification to the every bundle optical-fiber laser on the main optical path A, therefore use 5 couples of main optical path A of fiber amplifier to go up N bundle optical-fiber laser and carry out the light amplification of equal-wattage, make the laser after the coherent superposition that higher power be arranged, can use the fiber amplifier of 10W, thereby 10W power not significantly the nonlinear effect in the excitation fiber cause laser frequency to move, this has guaranteed that N bundle optical-fiber laser all has identical frequency, satisfy complete coherent condition, and the power of each bundle optical-fiber laser 10W is enough to obtaining high-power coherent laser.
The function of 90: 10 polarization-maintaining fiber couplers 6 is the optical-fiber laser beam splitting after amplifying through fiber amplifier 5,90% optical-fiber laser is exported from fiber end face, after lens 10 focus on,, obtain the coherent laser of high power and high light beam quality in the free space coherent superposition; 10% optical-fiber laser is by after being melted the identical light path of tapered polarization-maintaining fiber coupler 8 by 90: 10 polarization-maintaining fiber couplers 6 to 1 * 2, melt in the tapered polarization-maintaining fiber coupler 81 * 2 and to superpose with reference laser beam, the power of stack laser intensity has been reacted main optical path A and has been gone up between N bundle optical-fiber laser and the reference laser separately phase difference, the stack laser intensity is surveyed by avalanche photodide or PIN photodiode 11, and phase difference is changed into the control signal of telecommunication.This signal amplifies through feedback control circuit 9, acts on then on the fibre optic phase modulator 4, and the phase place and the reference laser phase place of the N bundle optical-fiber laser on the main optical path A are reached unanimity, and realizes main optical path A is gone up the phase locking of N bundle optical-fiber laser.
The function that 1 * N melts tapered polarization-maintaining fiber coupler 7 is, to melt the reference laser that tapered polarization-maintaining fiber coupler 3 obtains from 1 * N+1 and be divided into the N bundle, N bundle laser on the main optical path A that goes out with 10% beam splitting from 90: 10 polarization-maintaining fiber couplers 6 melts stack in the tapered polarization-maintaining fiber coupler 81 * 2 respectively, and the light after the stack sends avalanche photodide or PIN photodiode 11 in the feedback control circuit 9 to by secondary light path B.
1 * 2 function of melting tapered polarization-maintaining fiber coupler 8 is to make from 1 * N and melt tapered polarization-maintaining fiber coupler 7 reference laser that obtains and the optical-fiber laser stack of coming out from main optical path A polarization-maintaining fiber coupler 6 beam splitting in last 90: 10.Owing to have phase difference between the N bundle optical-fiber laser on the main optical path A, N bundle comprises the optical-fiber laser of 10% energy among the main optical path A and melts reference laser that tapered polarization-maintaining fiber coupler 7 obtains from 1 * N and melt the tapered polarization-maintaining fiber coupler 8 just difference to some extent of the light intensity after the stack 1 * 2, this difference reaction main optical path A go up phase difference between the N bundle optical-fiber laser.The reason that causes main optical path A to go up each laser beam phase difference comprises the influence of amplifier, the influence of fibre optic phase modulator, temperature fluctuation, each light path light path difference etc.
The function of feedback control circuit 9 is to survey from 1 * 2 to melt the power of the light of tapered polarization-maintaining fiber coupler 8, and converts thereof into the signal of telecommunication and act on the fibre optic phase modulator 4, and modulation main optical path A goes up N bundle optical-fiber laser phase place and reaches unanimity.Feedback control circuit 9 is made up of an avalanche photodide or PIN photodiode 11 and high-frequency amplifier 12.The function of avalanche photodide or PIN photodiode 11 is to survey 1 * 2 to melt the luminous intensity that sends in the tapered polarization-maintaining fiber coupler 8, converts the signal of telecommunication to through avalanche photodide or PIN photodiode 11.This signal of telecommunication acts on the fibre optic phase modulator 4 after amplifying through high-frequency amplifier 12, realizes that main optical path A is gone up N bundle optical-fiber laser implements the phase place regulation and control.As long as it is enough little that the response time of feedback control circuit 9 was compared with the coherence time of laser, just can realize main optical path A is gone up the good tracking and the control of N bundle optical-fiber laser phase place.Like this, the phase place of N on main optical path A bundle optical-fiber laser all with melt the reference laser phase place that tapered polarization-maintaining fiber coupler obtains from 1 * N+1 and reach unanimity, realized main optical path A is gone up the phase locking of N bundle optical-fiber laser, realized promptly that also main optical path A goes up the coherent superposition of N bundle optical-fiber laser at free space, thereby obtained phase locking multi-light beam coherent superimposed optical fiber laser.
The present invention has realized the complete coherent superposition of multiple beams of optical fiber laser, and the laser beam after the stack has high power and near the beam quality of diffraction limit.Use feedback control circuit 9, assurance is gone up N bundle optical-fiber laser phase place to main optical path A and is surveyed constantly and modulate, phase locking quality (coherence) can reach uniform and stable high level, thereby satisfies the complete coherent condition of N bundle optical-fiber laser, realizes relevant fully at output; Use 1 * N+1 to melt tapered polarization-maintaining fiber coupler 3, so the number of beams of coherent superposition optical-fiber laser is restricted hardly; Use polarization maintaining optical fibre isolator 2, when guaranteeing polarization state, reduced noise effect, increased the stability of a system; Use fibre optic phase modulator 4, fundamentally reduced the insertion loss and the echo reflection of device; Used the polarization maintaining optical fibre element in the system, realized the function that polarization exempts to regulate, also be beneficial to miniaturization, the practicability of system, easier commercial the application.Because the present invention realized output high-power and had the phase locking multiple beam stack output optical fibre laser of high light beam quality simultaneously, solved the shortcoming that the high power that exists in the existing fiber laser beam synthetic method and high light beam quality can not be taken into account.The fiber laser of this high power, high light beam quality can be applicable to ordinary optic fibre laser or the gas, solid, the semiconductor laser that have a tail optical fiber are changed into the LASER Light Source of output high-power, high light beam quality light, and many fields such as industrial lasers processing, military affairs.The fiber laser that the present invention is applicable to continuously or pulse is exported also is applicable to and mixes Tm 3+, Pr 3+, Ho 3+, Er 3+, Sm 3+, Nd 3+, Yb 3+The fiber laser of ion.Laser structure of the present invention is simple, compact, processing and manufacturing easily, is easy to industrial production.
Description of drawings:
Fig. 1 utilizes feedback loop to realize the multi-light beam coherent superimposed output optical fibre laser structure schematic diagram of phase locking.Fig. 1 also is the specification digest accompanying drawing.
The structural representation of Fig. 2 feedback control circuit 9.
Embodiment:
Embodiment 1:
Phase locking multi-light beam coherent superimposed optical fiber laser has been made in concrete enforcement.As shown in Figure 1, it comprises the fiber laser 1 of output polarization light, polarization maintaining optical fibre isolator 2,1 * N+1 melts tapered polarization-maintaining fiber coupler 3, fibre optic phase modulator 4, fiber amplifier 5,90: 10 polarization-maintaining fiber coupler 6,1 * N melt tapered polarization-maintaining fiber coupler 7,1 * 2 and melt tapered polarization-maintaining fiber coupler 8, feedback control circuit 9, lens 10.As shown in Figure 2, feedback control circuit 9 comprises avalanche photodide or PIN photodiode 11, high-frequency amplifier 12.The polarised light of output from fiber laser 1, melt tapered polarization-maintaining fiber coupler 3 through 1 * N+1 and be beamed into the N+1 bundle polarization laser that energy equates, wherein beam of laser is as the reference laser beam, it is melted tapered polarization-maintaining fiber coupler 7 by 1 * N again and is beamed into the N bundle polarization laser that energy equates, so as with main optical path A on 10% splitting optical fiber laser interference.Melt the other N bundle polarization fiber laser process fibre optic phase modulator 4 of tapered polarization-maintaining fiber coupler 3 beam splitting through 1 * N+1, amplified by fiber amplifier 5 then.Main optical path A goes up N bundle polarization laser after amplifying through polarization-maintaining fiber coupler 6 beam splitting in 90: 10,90% optical-fiber laser after lens 10 focus in the free space coherent superposition, the laser of output high-power and high light beam quality.10% polarization laser enters secondary light path B, on the secondary light path B with beam splitting after reference laser melt in the tapered polarization-maintaining fiber coupler 81 * 2 and interfere.Light after the interference enters feedback control circuit 9, the voltage control joint of fibre optic phase modulator 4 be connected with feedback control circuit 9 (as shown in Figure 2), avalanche photodide or PIN photodiode 11 are used for surveying 1 * 2 luminous intensity of melting in the tapered polarization-maintaining fiber coupler 8, and with the output of the form of the signal of telecommunication, this signal of telecommunication is after high-frequency amplifier 12 amplifies, be used for controlling fibre optic phase modulator 4, realize phase locking.

Claims (2)

1. phase locking multi-light beam coherent superimposed optical fiber laser, it is characterized in that it comprises the fiber laser (1) of output polarization light, polarization maintaining optical fibre isolator (2), 1 * N+1 melt tapered polarization-maintaining fiber coupler (3), fibre optic phase modulator (4), fiber amplifier (5), 90: 10 polarization-maintaining fiber couplers (6), 1 * N melts tapered polarization-maintaining fiber coupler (7), and 1 * 2 melts tapered polarization-maintaining fiber coupler (8), feedback control circuit (9), lens (10);
One end of polarization maintaining optical fibre isolator (2) connects the other end and melts tapered polarization-maintaining fiber coupler (3) with 1 * N+1 and connect with fiber laser (1); Fibre optic phase modulator (4) melts tapered polarization-maintaining fiber coupler (3) with 1 * N+1 and connects, also connects with fiber amplifier (5) and feedback control circuit (9); 90: 10 polarization-maintaining fiber coupler (6) connect with fiber amplifier (5) and also melt tapered polarization-maintaining fiber coupler (8) and lens (10) connect with 1 * 2; 1 * N melts tapered polarization-maintaining fiber coupler (7) and 1 * 2 and melts tapered polarization-maintaining fiber coupler (8) and connect, and links with feedback control circuit (9), also melts tapered polarization-maintaining fiber coupler (3) with 1 * N and connects.
2. a kind of phase locking multi-light beam coherent superimposed optical fiber laser according to claim 1 is characterized in that said feedback control circuit (9) is by avalanche photodide or PIN photodiode (11) and high-frequency amplifier (12) formation.
CNB2005100167725A 2005-04-30 2005-04-30 Phase locking multi-light beam coherent superimposed optical fiber laser Expired - Fee Related CN1331280C (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CNB2005100167725A CN1331280C (en) 2005-04-30 2005-04-30 Phase locking multi-light beam coherent superimposed optical fiber laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CNB2005100167725A CN1331280C (en) 2005-04-30 2005-04-30 Phase locking multi-light beam coherent superimposed optical fiber laser

Publications (2)

Publication Number Publication Date
CN1688069A true CN1688069A (en) 2005-10-26
CN1331280C CN1331280C (en) 2007-08-08

Family

ID=35306109

Family Applications (1)

Application Number Title Priority Date Filing Date
CNB2005100167725A Expired - Fee Related CN1331280C (en) 2005-04-30 2005-04-30 Phase locking multi-light beam coherent superimposed optical fiber laser

Country Status (1)

Country Link
CN (1) CN1331280C (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN100350684C (en) * 2005-11-23 2007-11-21 安徽大学 Frequency-modulation narrow-linewidth polarization-maintaining fiber laser
CN100405676C (en) * 2006-01-13 2008-07-23 中国科学院长春光学精密机械与物理研究所 High power density laser output optical fibre laser device
CN102263368A (en) * 2011-06-28 2011-11-30 北京交通大学 Multi-optical fiber passive phase-locking laser
CN102646916A (en) * 2012-05-02 2012-08-22 中国人民解放军国防科学技术大学 Coherent combination of high-power fiber laser full optical fiber structure and high brightness beam controlling method
CN107248693A (en) * 2017-06-08 2017-10-13 中国人民解放军武汉军械士官学校 A kind of adaptive drive device based on prism of corner cube coherent combining laser device

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3386090B2 (en) * 1994-02-23 2003-03-10 日本電信電話株式会社 Optical clock phase locked loop circuit
US5936980A (en) * 1996-09-26 1999-08-10 Lucent Technologies Inc. Internally modulated coupled cavity fiber lasers
US5894531A (en) * 1997-03-11 1999-04-13 Karta Technology, Inc. Method and apparatus for detection of ultrasound using a fiber-optic interferometer
US6310715B1 (en) * 2000-04-26 2001-10-30 The United States Of America As Represented By The United States Air Force Crystal stack for coherent optical beam combination

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN100350684C (en) * 2005-11-23 2007-11-21 安徽大学 Frequency-modulation narrow-linewidth polarization-maintaining fiber laser
CN100405676C (en) * 2006-01-13 2008-07-23 中国科学院长春光学精密机械与物理研究所 High power density laser output optical fibre laser device
CN102263368A (en) * 2011-06-28 2011-11-30 北京交通大学 Multi-optical fiber passive phase-locking laser
CN102646916A (en) * 2012-05-02 2012-08-22 中国人民解放军国防科学技术大学 Coherent combination of high-power fiber laser full optical fiber structure and high brightness beam controlling method
CN102646916B (en) * 2012-05-02 2015-05-13 中国人民解放军国防科学技术大学 Coherent combination of high-power fiber laser full optical fiber structure and high brightness beam controlling method
CN107248693A (en) * 2017-06-08 2017-10-13 中国人民解放军武汉军械士官学校 A kind of adaptive drive device based on prism of corner cube coherent combining laser device
CN107248693B (en) * 2017-06-08 2020-10-16 中国人民解放军武汉军械士官学校 Self-adaptive driving device based on pyramid prism coherent synthesis laser

Also Published As

Publication number Publication date
CN1331280C (en) 2007-08-08

Similar Documents

Publication Publication Date Title
CA2102644C (en) Spontaneous emission source having high spectral density at a desired wavelength
US6570704B2 (en) High average power chirped pulse fiber amplifier array
US7535628B2 (en) Laser light source, method of laser oscillation, and method of laser processing
US5243610A (en) Optical fiber dispersion-compensating device
US7599405B2 (en) Method and apparatus for coherently combining multiple laser oscillators
CN100578269C (en) Full fiber chirped pulse amplification system
KR100205052B1 (en) Mode locking optical fiber laser of wavelength tunable type
CN104300344A (en) High-power and tunable pulse fiber laser device
CN106451042A (en) Chirped pulse amplification system for fiber laser
US11870210B2 (en) Transverse mode switchable all-fiber high-order mode Brillouin laser
US6333803B1 (en) Optical transmitter
CN1331280C (en) Phase locking multi-light beam coherent superimposed optical fiber laser
JP5277761B2 (en) Optical semiconductor device and manufacturing method thereof
CN111555099A (en) Microwave generating system
CN212062984U (en) Microwave generating system
CN205666431U (en) Wavelength locking semiconductor laser
CN1556561A (en) Wave length tunable narrow wire width, high signal noise ratio single polarization ring cavity full optical fiber laser
EP3179645B1 (en) Optical signal modulation apparatus and system
US6400746B1 (en) Pump laser with low grating reflectivity
CN110544864A (en) Narrow linewidth fiber laser based on frequency modulation single-frequency seed source and four-wave mixing
US7433561B2 (en) All-optical phase, wavelength, and polarization-insensitive wavelength converters
CN204118459U (en) High power tunable pulse optical fiber
JP2012204372A (en) Short pulse light source and laser scanning microscope system
CN111725689A (en) Narrow linewidth fast tuning laser
CN113131322B (en) Mode locking fiber laser

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
C17 Cessation of patent right
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20070808