CN102967981A - Super-continuous spectrum light source based on multicore photonic crystal fiber - Google Patents
Super-continuous spectrum light source based on multicore photonic crystal fiber Download PDFInfo
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- CN102967981A CN102967981A CN2012105516154A CN201210551615A CN102967981A CN 102967981 A CN102967981 A CN 102967981A CN 2012105516154 A CN2012105516154 A CN 2012105516154A CN 201210551615 A CN201210551615 A CN 201210551615A CN 102967981 A CN102967981 A CN 102967981A
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Abstract
The invention provides a super-continuous spectrum light source based on a multicore photonic crystal fiber, which comprises a pump laser with an output pigtail, and a multicore photonic crystal fiber. The output pigtail of the selected pump laser is welded with an input end of the multicore photonic crystal fiber with matched mode field and a dispersion characteristic to form a whole-fiber super-continuous spectrum light source. The multicore photonic crystal fiber with larger mode field area and adjustable dispersion characteristic can be taken as a generating medium of the super-continuous spectrum, which effectively solves the problems that the normal single-core photonic crystal fiber as the generating medium of the super-continuous spectrum is difficult to weld with the pump laser, and the dispersion characteristic of the photonic crystal fiber is not matched with the operating wavelength of the pump laser, when generating the high-average power whole-fiber super-continuous spectrum, can effectively realize output of the high-average power whole-fiber super-continuous spectrum, and at the same time, greatly improve the power upper limit of the system.
Description
Technical field
The present invention relates to the Fiber laser technology field, refer in particular to a kind of light source that can realize the full fiberize super continuous spectrums output of high-average power.
Background technology
At present, the low-power super continuum source that adopts optical-fiber laser pump photon crystal optical fibre to realize has become a kind of practical commodity.But some application need to have the super continuum source of high average output power and high spectral concentration, and existing super continuum source still can not satisfy the demands.
Super continuum source generally comprises pumping source and super continuous spectrums produces medium two parts.The super continuous spectrums form that the characteristic (dispersion characteristics, nonlinear response) of the parameter of pumping laser (operation wavelength, pulse width, pulse peak power) and nonlinear medium has determined that jointly which kind of nonlinear effect can occur and finally exported.In fact the small differences of the parameter of pumping source and optic fibre characteristic can make a significant impact the spectrum of super continuous spectrums production process and final output, and the characteristic of only having nonlinear medium can produce more satisfactory super continuous spectrums during with the pumping source comparison match.
At present, the super continuous spectrums of acquisition high average output power and high spectral concentration mainly is to utilize the single core photonic crystal fiber of high power optical fibre laser pumping of technology comparative maturity to carry out.For realizing the very big broadening of super continuum light spectrum, require the pumping laser operation wavelength should be chosen in the anomalous dispersion region of close photonic crystal fiber zero dispersion point.But the core diameter of the output tail optical fiber in high power pump source is generally all greater than 10 microns, the core diameter of the photonic crystal fiber that dispersion characteristics match is less than 10 microns, exist larger mould field not mate between the two, this is so that high power pump laser is very difficult to the coupling of photonic crystal fiber.Although can reduce by the core diameter that increases single core photonic crystal fiber the mould field does not mate, but this can reduce the nonlinear factor of single core photonic crystal fiber on the one hand, also can change on the other hand the dispersion characteristics of photonic crystal fiber, be unfavorable for the generation of super continuous spectrums.The optical conversion efficiencies that the larger coupling loss that causes can reduce system is not mated in the mould field, more seriously the excessive fire damage that also can cause fusion point of coupling loss.Even the coupled problem of high power pump laser is solved, because the mode field diameter less of single core photonic crystal fiber, the factors such as thermal effect and damage from laser have also fundamentally limited the output power based on the super continuum source of single core photonic crystal fiber.
In recent years, the concept of multicore photonic crystal optical fiber is suggested.Light field between each fibre core of multicore photonic crystal optical fiber intercouples and can form what is called " super model ", and homophase super model wherein has the far-field intensity distribution of class Gaussian, and effectively mould field distribution area is larger, and its mould field distribution is insensitive to heat and stress.In addition, the dispersion characteristics of multicore photonic crystal optical fiber super model are less with the dispersion characteristics difference of the single core photonic crystal fiber with same air packing ratio.So multicore photonic crystal optical fiber can have the dispersion characteristics with the pumping laser comparison match when having than big mode field area.Have the document proof to adopt multicore photonic crystal optical fiber can realize the generation of super continuous spectrums, but pumping laser all is to adopt the Lens Coupling mode to enter into photonic crystal fiber in these documents, this has reduced Systems balanth, is unfavorable for practical application.At present, the granted patent bulletin that existing continuous spectrum light source is relevant, but the patent that adopts multicore photonic crystal optical fiber to produce medium as super continuous spectrums is not yet arranged.
Summary of the invention
Existing based on the deficiency in the super continuous spectrums generating technique of single core photonic crystal fiber for overcoming, promote the average output power of super continuum source, the present invention proposes a kind of super continuum source based on multicore photonic crystal optical fiber, can realize the full fiberize super continuous spectrums output of high-average power.
Pump laser and multicore photonic crystal optical fiber two parts that the super continuum source based on multicore photonic crystal optical fiber that the present invention proposes is exported tail optical fiber by band form, the input end of the multicore photonic crystal optical fiber of isotype of the output tail optical fiber of the pump laser of selecting and dispersion characteristics coupling is carried out welding, namely consisted of the super continuum source of full fiberize.
Described pump laser is: the dispersion characteristics of operation wavelength and multicore photonic crystal optical fiber are complementary; The output of band tail optical fiber, and the good beam quality of the laser of exporting from tail optical fiber are for fundamental transverse mode or near fundamental transverse mode; The mould field of the mould field of output tail optical fiber and the super model of multicore photonic crystal optical fiber is complementary; Output of laser enters into multicore photonic crystal optical fiber can excite super continuous spectrums effectively.
Described pump laser is rare-earth ion-doped (ytterbium, erbium, thulium, holmium, bismuth etc.) fiber laser or based on the fiber laser (Raman fiber lasers of nonlinear effect, parameteric light fibre laser etc.), or solid state laser, or semiconductor laser, by coupled system Output of laser is coupled in the optical fiber, consists of the pump laser of band output tail optical fiber.
The working method of pump laser can be the pulse laser operation, also can be the continuous wave laser operation.
Described multicore photonic crystal optical fiber is that super continuous spectrums produces medium, can form stable homophase super model, and support its low-loss transmission; The dispersion characteristics of multicore photonic crystal optical fiber and the operation wavelength of pump laser are complementary; The mould field of the mould field of the homophase super model of multicore photonic crystal optical fiber and the output tail optical fiber of pumping laser is complementary; Have nonlinear characteristic, satisfy power condition and namely satisfy and to produce the super continuous spectrums condition.
The characteristic of described multicore photonic crystal optical fiber realizes by design optical fiber, the design photonic crystal fiber mainly is the end face structure of considering optical fiber, and the end face of multicore photonic crystal is comprised of optical fiber base material, fibre core and the hole different from optical fiber base material refractive index.By changing the refractive index of various piece, physical dimension and arrangement mode can be realized different optic fibre characteristics.
The base material of described multicore photonic crystal optical fiber will carry out choose reasonable according to the wave band of required super continuous spectrums, comprise pure quartz (mainly producing visible light and near-infrared band super continuous spectrums), telluride, sulfide and fluoride materials (mainly producing the infrared band super continuous spectrums).
The fibre core number of described multicore photonic crystal optical fiber is not strict with (can be seven cores, 19 cores or other number).The refractive index of fibre core can be identical with the optical fiber base material, also can be different.The refractive index of each fibre core can be identical with geometric configuration, also can be different.Can doped rare earth element in the material of fibre core, can not mix yet.
The hole of described multicore photonic crystal optical fiber end face can be airport, also can be filled by other high-index material.The shape in single hole can be circular, oval or other shape, and the shape in each hole and other hole can be the same, also can be different.It can be the arbitrary shape (regular hexagon, octagon, dodecagon, circle etc.) that allows that the integral body in hole is arranged.
The external diameter of described multicore photonic crystal optical fiber vertically can be uniformly along optical fiber, also can be non-homogeneous.
When the output tail optical fiber of described pump laser carries out welding with the input end of multicore photonic crystal optical fiber, can use the photonic crystal fiber post-processing technology, the photonic crystal fiber end face is processed, further reduce splice loss, splice attenuation.
The invention has the advantages that: adopt to have than big mode field area, the adjustable multicore photonic crystal optical fiber of dispersion characteristics is as the generation medium of super continuous spectrums, efficiently solve conventional adopt the single-core fiber crystal optical fibre as the generation medium of super continuous spectrums when realizing that the full fiberize super continuous spectrums of high-average power produces, the pumping laser coupling difficulty that exists, the dispersion characteristics of photonic crystal fiber and pumping laser operation wavelength such as do not mate at the problem, can effectively realize the full fiberize super continuous spectrums output of high-average power, greatly promote the power upper limit of system simultaneously.This light source also utilizes ripe high power optical fibre laser technology, photonic crystal fiber manufacturing technology and photonic crystal fiber post-processing technology, simplified the system architecture of the full fiberize super continuum source of high-average power, reduce system cost, be convenient to suitability for industrialized production and application.
Description of drawings
Fig. 1 is the structural representation based on the super continuum source of multicore photonic crystal optical fiber that the present invention proposes,
Fig. 2 is the end face structure synoptic diagram of the multicore photonic crystal optical fiber that adopts in a kind of specific embodiment.
Embodiment
Among the figure: the pump laser of 1-band output tail optical fiber; The 2-multicore photonic crystal optical fiber; The output tail optical fiber 3 of 3-pump laser; The 4-fusion point; The base material of 5-photonic crystal fiber; The fibre core of 6-photonic crystal fiber; The 7-aperture.
The present invention is described in further detail below in conjunction with accompanying drawing and specific embodiment.Specific embodiment described herein only is used for explaining the present invention, but should limit protection scope of the present invention with this.
Fig. 1 is the structural representation based on the super continuum source of multicore photonic crystal optical fiber that the present invention proposes.As shown in the figure, the super continuum source that the present invention proposes comprises the pump laser 1 of band output tail optical fiber, multicore photonic crystal optical fiber 2, wherein, the output tail optical fiber 3 of pump laser 1 carries out welding with an end face of multicore photonic crystal optical fiber 2 and consists of all optical fibre structure, fusion point 4.When pumping laser is coupled into the multicore photonic crystal optical fiber 2 that matches, because the effect of various nonlinear effects forms super continuous spectrums in multicore photonic crystal optical fiber 2, the super continuous spectrums of generation is from another end face output of multicore photonic crystal optical fiber 2.
In a kind of specific embodiment of the present invention, pump laser 1 adopts the picopulse ytterbium-doping optical fiber laser, its operation wavelength is near 1.06 microns, pulse width is about 20 psecs, pulse repetition rate is 500 megahertzes, average power is 56 watts, and output tail optical fiber 3 is 15 microns of core diameters, the doubly clad optical fiber that the inner cladding diameter is 130 microns; This pump laser is that basic mode distributes from the light field of the laser of tail optical fiber output.
Fig. 2 is the end face structure synoptic diagram of the multicore photonic crystal optical fiber that adopts among this embodiment.This multicore photonic crystal optical fiber is seven core fibre crystal optical fibres, the base material 5 of photonic crystal fiber is pure quartz, the fibre core 6 of photonic crystal fiber is positive hexagon, 7 one-tenth arranged in regular hexagon shapes of aperture on the end face, and all be that bore dia is 1.49 microns circular airport, the pitch of holes in two holes of arbitrary neighborhood is 3.26 microns, and fibre core is to form by an airport cancelling correspondence position.The external diameter of multicore photonic crystal optical fiber vertically is that length is 20 m uniformly along optical fiber among the embodiment;
Under maximum pumping laser power, the super continuum source output average power based on multicore photonic crystal optical fiber among this embodiment is 40 W, and spectral range is the super continuous spectrums of 600-1700 nanometers, and output light field is that the homophase super model distributes.
Claims (9)
1. based on the super continuum source of multicore photonic crystal optical fiber, the pump laser and the multicore photonic crystal optical fiber that comprise band output tail optical fiber, it is characterized in that, the input end of the multicore photonic crystal optical fiber of isotype of the output tail optical fiber of the pump laser of selecting and dispersion characteristics coupling is carried out welding, namely consisted of the super continuum source of full fiberize;
Described pump laser is: the dispersion characteristics of operation wavelength and multicore photonic crystal optical fiber are complementary; The output of band tail optical fiber, and the good beam quality of the laser of exporting from tail optical fiber are for fundamental transverse mode or near fundamental transverse mode; The mould field of the mould field of output tail optical fiber and the homophase super model of multicore photonic crystal optical fiber is complementary; Output of laser enters into multicore photonic crystal optical fiber can excite super continuous spectrums effectively;
Described multicore photonic crystal optical fiber is that super continuous spectrums produces medium, can form stable homophase super model, and support its low-loss transmission; The dispersion characteristics of multicore photonic crystal optical fiber and the operation wavelength of pump laser are complementary; The mould field of the mould field of the homophase super model of multicore photonic crystal optical fiber and the output tail optical fiber of pumping laser is complementary; Have nonlinear characteristic, satisfy power condition and can produce the super continuous spectrums condition.
2. the super continuum source based on multicore photonic crystal optical fiber according to claim 1, it is characterized in that, described pump laser is rare-earth ion-doped, comprise the fiber laser of ytterbium, erbium, thulium, holmium, bismuth or based on the fiber laser of nonlinear effect, comprise Raman fiber lasers, parameteric light fibre laser, perhaps solid state laser, perhaps semiconductor laser, by coupled system Output of laser is coupled in the optical fiber, consists of the pump laser of band output tail optical fiber.
3. the super continuum source based on multicore photonic crystal optical fiber according to claim 1 is characterized in that, the working method of pump laser can be the pulse laser operation, also can be the continuous wave laser operation.
4. the super continuum source based on multicore photonic crystal optical fiber according to claim 1, it is characterized in that, the end face of described multicore photonic crystal optical fiber is comprised of optical fiber base material, fibre core and the hole different from optical fiber base material refractive index, change the refractive index of various piece, physical dimension and arrangement mode can be realized different optic fibre characteristics.
5. the super continuum source based on multicore photonic crystal optical fiber according to claim 1 is characterized in that, the base material of described multicore photonic crystal optical fiber comprises pure quartz, telluride, sulfide and fluoride materials.
6. the super continuum source based on multicore photonic crystal optical fiber according to claim 1 is characterized in that, the fibre core number of described multicore photonic crystal optical fiber can be seven cores, 19 cores or other number; The refractive index of fibre core can be identical with the optical fiber base material, also can be different; The refractive index of each fibre core can be identical with geometric configuration, also can be different; Can doped rare earth element in the material of fibre core, can not mix yet.
7. the super continuum source based on multicore photonic crystal optical fiber according to claim 1 is characterized in that, the hole of described multicore photonic crystal optical fiber end face can be airport, also can be filled by other high-index material; The shape in single hole can be circular, oval or other shape, and the shape in each hole and other hole can be the same, also can be different; It can be the arbitrary shape that allows that the integral body in hole is arranged.
8. the super continuum source based on multicore photonic crystal optical fiber according to claim 1 is characterized in that, the external diameter of described multicore photonic crystal optical fiber vertically can be uniformly along optical fiber, also can be non-homogeneous.
9. the super continuum source based on multicore photonic crystal optical fiber according to claim 1, it is characterized in that, when the output tail optical fiber of described pump laser carries out welding with the input end of multicore photonic crystal optical fiber, can use the photonic crystal fiber post-processing technology, the photonic crystal fiber end face is processed, further reduced splice loss, splice attenuation.
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Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103293678A (en) * | 2013-06-04 | 2013-09-11 | 中国人民解放军国防科学技术大学 | Even laser illuminating device based on supercontinuum source |
| CN103296566A (en) * | 2013-06-01 | 2013-09-11 | 中国人民解放军国防科学技术大学 | Method for increasing power proportion of supercontinuum long waves in fluoride fiber |
| CN103487879A (en) * | 2013-09-23 | 2014-01-01 | 北京工业大学 | Seven-core photonic crystal fiber for restraining high-order super-mode output |
| CN105896252A (en) * | 2016-06-12 | 2016-08-24 | 中国人民解放军国防科学技术大学 | High-power visible light enhanced super-continuum spectrum light source |
| CN106125193A (en) * | 2016-09-13 | 2016-11-16 | 电子科技大学 | A kind of sulfide photonic crystal fiber |
| CN106255907A (en) * | 2014-03-25 | 2016-12-21 | Nkt光子学有限公司 | Microstructured optical fibers and super continuum source |
| CN108181723A (en) * | 2018-01-30 | 2018-06-19 | 电子科技大学 | It is a kind of based on close coupling multi-core optical fiber Random Laser without speckle imaging source |
| CN109818241A (en) * | 2019-01-14 | 2019-05-28 | 中国工程物理研究院激光聚变研究中心 | A kind of high power super continuous spectrum laser system |
| CN112152056A (en) * | 2019-06-28 | 2020-12-29 | 中国科学院上海光学精密机械研究所 | Full-fiber large-energy supercontinuum laser |
| CN112242640A (en) * | 2019-07-19 | 2021-01-19 | 中国科学院上海光学精密机械研究所 | Supercontinuum light source based on high-power multimode laser and super multi-core high-nonlinearity optical fiber |
Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101770132A (en) * | 2008-12-31 | 2010-07-07 | 中国科学院西安光学精密机械研究所 | Visible light strengthened super continuous spectrum laser system with all-optical-fiber structure |
| CN101819086A (en) * | 2010-05-19 | 2010-09-01 | 中国人民解放军国防科学技术大学 | Optical fiber dispersion measurement system and use method thereof |
| CN101969175A (en) * | 2010-09-29 | 2011-02-09 | 天津大学 | Ytterbium-doped multicore photonic crystal optical fiber mode-locked laser |
| CN102401934A (en) * | 2010-09-10 | 2012-04-04 | 北京邮电大学 | Flattened dispersion photonic crystal optical fiber |
| CN202995205U (en) * | 2012-12-18 | 2013-06-12 | 中国人民解放军国防科学技术大学 | Multicore photonic crystal fiber based supercontinuum source |
-
2012
- 2012-12-18 CN CN2012105516154A patent/CN102967981A/en active Pending
Patent Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101770132A (en) * | 2008-12-31 | 2010-07-07 | 中国科学院西安光学精密机械研究所 | Visible light strengthened super continuous spectrum laser system with all-optical-fiber structure |
| CN101819086A (en) * | 2010-05-19 | 2010-09-01 | 中国人民解放军国防科学技术大学 | Optical fiber dispersion measurement system and use method thereof |
| CN102401934A (en) * | 2010-09-10 | 2012-04-04 | 北京邮电大学 | Flattened dispersion photonic crystal optical fiber |
| CN101969175A (en) * | 2010-09-29 | 2011-02-09 | 天津大学 | Ytterbium-doped multicore photonic crystal optical fiber mode-locked laser |
| CN202995205U (en) * | 2012-12-18 | 2013-06-12 | 中国人民解放军国防科学技术大学 | Multicore photonic crystal fiber based supercontinuum source |
Non-Patent Citations (2)
| Title |
|---|
| XIAO-HUI FANG 等: "Multiwatt octave-spanning supercontinuum generation in multicore photonic-crystal fiber", 《OPTICS LETTERS》 * |
| 谌鸿伟 等: "国产光子晶体光纤实现4.6 W 全光纤超连续谱输出", 《光学学报》 * |
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| CN103296566A (en) * | 2013-06-01 | 2013-09-11 | 中国人民解放军国防科学技术大学 | Method for increasing power proportion of supercontinuum long waves in fluoride fiber |
| CN103293678B (en) * | 2013-06-04 | 2015-04-08 | 中国人民解放军国防科学技术大学 | Even laser illuminating device based on supercontinuum source |
| CN103293678A (en) * | 2013-06-04 | 2013-09-11 | 中国人民解放军国防科学技术大学 | Even laser illuminating device based on supercontinuum source |
| CN103487879B (en) * | 2013-09-23 | 2015-08-05 | 北京工业大学 | A kind of seven core photonic crystal fibers suppressing high-order super model to export |
| CN103487879A (en) * | 2013-09-23 | 2014-01-01 | 北京工业大学 | Seven-core photonic crystal fiber for restraining high-order super-mode output |
| CN110989071B (en) * | 2014-03-25 | 2022-04-08 | Nkt光子学有限公司 | Microstructured optical fiber and supercontinuum light source |
| CN106255907A (en) * | 2014-03-25 | 2016-12-21 | Nkt光子学有限公司 | Microstructured optical fibers and super continuum source |
| EP3123216B1 (en) * | 2014-03-25 | 2023-10-25 | NKT Photonics A/S | A source of optical supercontinuum generation comprising a microstructured optical fiber |
| US10274672B2 (en) | 2014-03-25 | 2019-04-30 | Nkt Photonics A/S | Microstructured fiber and supercontinuum light source |
| US11619778B2 (en) | 2014-03-25 | 2023-04-04 | Nkt Photonics A/S | Source of supercontinuum radiation and microstructured fiber |
| CN106255907B (en) * | 2014-03-25 | 2020-01-24 | Nkt光子学有限公司 | Microstructured optical fiber and supercontinuum light source |
| CN110989071A (en) * | 2014-03-25 | 2020-04-10 | Nkt光子学有限公司 | Microstructured optical fiber and supercontinuum light source |
| US10698155B2 (en) | 2014-03-25 | 2020-06-30 | Nkt Photonics A/S | Microstructured fiber and supercontinuum light source |
| CN105896252A (en) * | 2016-06-12 | 2016-08-24 | 中国人民解放军国防科学技术大学 | High-power visible light enhanced super-continuum spectrum light source |
| CN105896252B (en) * | 2016-06-12 | 2019-04-09 | 中国人民解放军国防科学技术大学 | High power visible light strengthened super continuous spectrum light source |
| CN106125193A (en) * | 2016-09-13 | 2016-11-16 | 电子科技大学 | A kind of sulfide photonic crystal fiber |
| CN108181723B (en) * | 2018-01-30 | 2019-09-03 | 电子科技大学 | It is a kind of based on close coupling multi-core optical fiber Random Laser without speckle imaging source |
| CN108181723A (en) * | 2018-01-30 | 2018-06-19 | 电子科技大学 | It is a kind of based on close coupling multi-core optical fiber Random Laser without speckle imaging source |
| CN109818241A (en) * | 2019-01-14 | 2019-05-28 | 中国工程物理研究院激光聚变研究中心 | A kind of high power super continuous spectrum laser system |
| CN109818241B (en) * | 2019-01-14 | 2023-11-17 | 中国工程物理研究院激光聚变研究中心 | High-power supercontinuum laser system |
| CN112152056A (en) * | 2019-06-28 | 2020-12-29 | 中国科学院上海光学精密机械研究所 | Full-fiber large-energy supercontinuum laser |
| CN112152056B (en) * | 2019-06-28 | 2022-05-31 | 中国科学院上海光学精密机械研究所 | Full-fiber large-energy supercontinuum laser |
| CN112242640A (en) * | 2019-07-19 | 2021-01-19 | 中国科学院上海光学精密机械研究所 | Supercontinuum light source based on high-power multimode laser and super multi-core high-nonlinearity optical fiber |
| CN112242640B (en) * | 2019-07-19 | 2022-01-28 | 中国科学院上海光学精密机械研究所 | Supercontinuum light source based on high-power multimode laser and super multi-core high-nonlinearity optical fiber |
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