CN203014156U - High-power high-efficiency super-continuous spectrum light source - Google Patents
High-power high-efficiency super-continuous spectrum light source Download PDFInfo
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- CN203014156U CN203014156U CN 201220702770 CN201220702770U CN203014156U CN 203014156 U CN203014156 U CN 203014156U CN 201220702770 CN201220702770 CN 201220702770 CN 201220702770 U CN201220702770 U CN 201220702770U CN 203014156 U CN203014156 U CN 203014156U
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Abstract
The utility model provides a high-power high-efficiency super-continuous spectrum light source. The characteristics of photonic crystal fibers are reasonably designed, long-pulse pumping laser (picoseconds, nanosecond laser) is applied to a photonic crystal fiber normal dispersion area, enabling central wavelengths of previously excited of Raman Stokes peaks to be located close to an abnormal dispersion area of a zero dispersion points of the photonic crystal fibers, and an excited Raman Stokes laser peak acts as a new pumping source for exciting a super-continuous spectrum, and satisfies an abnormal dispersion pumping mechanism. The super-continuous spectrum light source has the advantages of both a normal dispersion pumping mechanism and an abnormal dispersion pumping mechanism, and can realize high average output power, high optical conversion efficiency and relatively wide continuous spectrum output in a super-continuous spectrum range. The light source utilizes mature high power fiber laser technology, photonic crystal fiber manufacturing technology and photonic crystal fiber postprocessing technology, reducing system cost, and facilitating industrialized production and application.
Description
Technical field
The present invention relates to the Fiber laser technology field, refer in particular to and a kind ofly can realize high average output power, the full fiberize super continuum source that high optical conversion efficiencies and output spectrum are relatively wide.
Background technology
Photonic crystal fiber can have again dispersion characteristics flexibly when satisfying the required high non-linearity of generation super continuous spectrums, utilize photonic crystal fiber can produce the super continuous spectrums of function admirable.Estimate a super continuum source, many indexs are arranged: the scope of super continuous spectrums, the flatness of super continuous spectrums, the average output power of super continuous spectrums, the spectral power density of super continuous spectrums, the coherence of super continuous spectrums, the output beam quality of super continuous spectrums etc.Different applications also can be given priority to for the performance requirement of super continuum source.At present, the granted patent bulletin that existing super continuum source is relevant, but being the Chinese patent of CN 201147308 Y, notification number reported the light source that is used for the super continuous spectrums of optical coherence tomography, notification number is the light source that the Chinese patent of CN 201332211 Y is paid close attention to the super continuous spectrums of visible light wave range enhancing, notification number is the flatness that the Chinese patent of CN 101825826 B is more emphasized super continuous spectrums, and notification number is the pump laser that the Chinese patent of CN 202487963 U is more paid attention to the selective exitation super continuous spectrums.But some application need to be used the super continuous spectrums with high average output power and high spectral concentration.In addition, the optical conversion efficiencies of super continuum source is also very important, and higher optical conversion efficiencies can reduce the requirement to pumping laser, can also reduce system cost.
Produce relevant nonlinear effect to super continuous spectrums and mainly comprise from phase-modulation, intersection position modulation, modulation is unstable, four wave mixing, stimulated Raman scattering, orphan's decomposition, orphan's self-frequency shift, dispersive wave produces, and orphan's (dispersive wave) catches, light pulse decomposition etc.The super continuous spectrums form that the characteristic (dispersion characteristics, nonlinear response) of the parameter of pumping laser (operation wavelength, pulse duration, pulse peak power) and nonlinear dielectric has determined that jointly which kind of nonlinear effect can occur and finally exported.According to the pulse duration of pumping laser and the dispersion characteristics of nonlinear dielectric, the super continuous spectrums production process roughly can be divided into following four kinds of situations: paper short pulse (subpicosecond magnitude) pumping laser acts on the situation of nonlinear dielectric the anomalous dispersion region, and the generation of super continuous spectrums in this case mainly is based on the effect that the orphan is correlated with.Because peak power is enough high, pumping pulse generally can be thought higher-order soliton.Because of the disturbance of the factors such as high-order dispersion and stimulated Raman scattering, higher-order soliton can resolve into a series of fundamental soliton in transmitting procedure.Due to the effect of Raman scattering effect in pulse, the red shift constantly of the spectrum of fundamental soliton.Simultaneously, the orphan also is accompanied by the generation of the blue shift dispersive wave of shortwave direction coupling in transmitting procedure.At last, be coupled by the Cross-phase Modulation effect between the Raman soliton of generation and the dispersive wave of Group-velocity Matching, the super continuous spectrums of generation is further expanded to shortwave and long wave.(pulsewidth is psec to the pumping laser long for pulsewidth, nanosecond is continuous light even) act on the situation of nonlinear dielectric the anomalous dispersion region, caused the soliton order of pumping laser very large because long pulse is wide, the characteristic length that the orphan decomposes becomes very long, considerably beyond the fiber lengths of actual use.Therefore, in this case, orphan's destructive effect is also not obvious in the initial production process of super continuous spectrums.Modulate unstable effect (four-wave mixing effect) and replace, dominated the initial production process of super continuous spectrums.Pumping pulse is resolved into a series of subpulse by the unstable process effect of modulation on time domain.It is the same that follow-up super continuous spectrums broadening process just acts on the situation of nonlinear dielectric the anomalous dispersion region with the short pulse pumping laser in essence; Each subpulse can experience the orphan and decompose, orphan's self-frequency shift, the processes such as dispersive wave generation.
Act on the situation in nonlinear dielectric normal dispersion district for the short pulse pumping laser, dominated the initial broadening of spectrum from phase-modulation.The pulse of pumping pulse is narrower, and Spectral Broadening is just wider.For long pulse pumping laser effect situation, the initial spectrum broadening has benefited from four wave mixing and Raman scattering process.If pumping wavelength from the zero dispersion point of photonic crystal fiber away from the time, the parameter sideband of parametric process and the off resonance of pumping wavelength are excessive, Raman scattering process will be dominated the broadening of spectrum.If pumping wavelength is during near the zero dispersion point of photonic crystal fiber, the effect of four-wave mixing effect is more obvious, because the gain of four-wave mixing effect is greater than Raman gain.For the situation of normal dispersion district's pumping, when the zero dispersion point that the spectrum of broadening is crossed photonic crystal fiber entered into the anomalous dispersion region, soliton mechanism can play a role again, and will dominate gradually the spectrum widening process of whole super continuous spectrums.In general, the scope that pumping laser acts on the super continuum light spectrum that the nonlinear dielectric the anomalous dispersion region produces likens to for normal dispersion district situation wide, particularly the super continuous spectrums of shortwave direction.
Related Mechanism according to super continuous spectrums produces for realizing the very big broadening of super continuum light spectrum, requires 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 makes high power pump laser very difficult to the coupling of photonic crystal fiber, has limited the lifting of super continuum source power output.
Adopt operation wavelength to be positioned at the laser in normal dispersion district of photonic crystal fiber as pumping source, can produce super continuous spectrums equally, although the super continuum light spectral limit that produces is relatively narrow based on the super continuum source that adopts the anomalous dispersion pumping mechanism, it has the advantage of oneself.Have the document record to adopt the normal dispersion pumping mechanism can realize that high efficiency super continuous spectrums produces, but do not adopt all optical fibre structure in experiment, this has reduced Systems balanth, is unfavorable for practical application.In addition, if adopt the normal dispersion pumping mechanism, can produce super continuous spectrums with the relatively large photonic crystal fiber of core diameter.Does not mate the mould field that has so just reduced between photonic crystal fiber and pumping optical fiber Laser output tail optical fiber, can be coupled more high-power pumping laser in photonic crystal fiber, promotes the power output of super continuum source.
Summary of the invention
Existing based on the deficiency in the super continuous spectrums generating technique of photonic crystal fiber for overcoming, the present invention proposes a kind ofly can realize high average output power, high optical conversion efficiencies and and the relatively wide full fiberize super continuum source of output spectrum.
The super continuum source that the present invention proposes is by the pump laser of band output tail optical fiber, and photonic crystal fiber two parts form.The output tail optical fiber of the pump laser of selecting is carried out welding with the input of photonic crystal fiber, namely consisted of the super continuum source of full fiberize.
Its operation principle is: by the characteristic of appropriate design photonic crystal fiber, adopt long pulse pumping laser (psec, nanosecond) to act on photonic crystal fiber normal dispersion district, the initial broadening of the leading spectrum of Raman scattering process; And the centre wavelength that makes the Raman Stokes peak of front what (is preferably first or the second level) that excites is positioned at the anomalous dispersion region near the zero dispersion point of photonic crystal fiber, the Raman Stokes laser peak that excites is just as exciting a new pumping source of super continuous spectrums, and satisfies the anomalous dispersion pumping mechanism; Reasonably optimize fiber lengths with crossing, make that the excited Raman effect can both effectively excite in the fiber lengths scope of using, the energy that guarantees pumping laser can both be transferred to Raman Stokes laser peak.This super continuum source has the advantage of normal dispersion pumping mechanism and anomalous dispersion pumping mechanism concurrently, can realize full fiberize super continuous spectrums output high-power high-efficiency, that the super continuum light spectrum is relatively wide.
Described pump laser is: operation wavelength is positioned at the normal dispersion district of photonic crystal fiber, and when it acted on photonic crystal fiber, the centre wavelength at front what the Raman Stokes laser peak that excites was positioned at the anomalous dispersion region near the zero dispersion point of photonic crystal fiber; Pumping laser used should be long pulse pumping laser (psec or ps pulsed laser and ns pulsed laser); 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; Output of laser enters into photonic crystal fiber can excite super continuous spectrums effectively.
Described pump laser can be for rare-earth ion-doped (ytterbium, erbium, thulium, holmium, bismuth etc.) fiber laser or based on the fiber laser (Raman fiber lasers of nonlinear effect, the parameteric light fibre laser), also can be solid state laser or semiconductor laser, by coupled system, Output of laser is coupled in optical fiber, consists of the pump laser of band output tail optical fiber.
Described photonic crystal fiber is that super continuous spectrums produces medium.Requirement to photonic crystal fiber is: the characteristic of photonic crystal fiber needs particular design, makes the centre wavelength at front what Raman Stokes laser peak of pumping laser be positioned at the anomalous dispersion region near the zero dispersion point of photonic crystal fiber; Have certain nonlinear characteristic, satisfy certain power condition and can produce super continuous spectrums.
The characteristic of described photonic crystal fiber can realize by appropriate design optical fiber, and the design photonic crystal fiber is mainly the end face structure of considering optical fiber.The end face of photonic crystal is by the optical fiber base material, and fibre core forms with 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 photonic crystal fiber will carry out choose reasonable according to the wave band of required super continuous spectrums, can be pure quartz (mainly producing visible light and near infrared band super continuous spectrums), can be also tellurides, sulfide and fluoride materials (mainly producing the infrared band super continuous spectrums).
The refractive index of the fibre core of described photonic crystal fiber can be identical with the optical fiber base material, also can be different.The refractive index of each fibre core and geometry can be identical, also can be different.Can doped rare earth element in the material of fibre core, can not mix yet.
The hole of described photonic crystal fiber end face can be airport, also can be filled by other high-index material.The shape in single hole can be circular, ellipse or other shape, and each hole can be the same with other hole, 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 optimization of described length to photonic crystal fiber is mainly to consider how pump light excites Raman stokes spectrum peak effectively, when particularly pumping laser is picosecond laser, walk-off effect is larger on the impact of excited Raman effect, and walking from length of fiber lengths and pulse is basically identical.
The external diameter of described photonic crystal fiber can be vertically uniformly along optical fiber, can be also non-homogeneous.
When the output tail optical fiber of described pump laser carries out welding with the input of photonic crystal 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 photonic crystal fiber post-processing technology has document " post-processing technology of photonic crystal fiber " record.
The invention has the advantages that: the present invention proposes a kind of full fiberize super continuum source, and by the pump laser of band output tail optical fiber, photonic crystal fiber two parts form.Characteristic by the appropriate design photonic crystal fiber, adopt long pulse pumping laser (psec, nanosecond laser) act on photonic crystal fiber normal dispersion district, and make front what the centre wavelength at Raman Stokes peak that excites be positioned at the anomalous dispersion region near the zero dispersion point of photonic crystal fiber, the Raman Stokes laser peak that excites is just as exciting a new pumping source of super continuous spectrums, and satisfies the anomalous dispersion pumping mechanism.This super continuum source has the advantage of normal dispersion pumping mechanism and anomalous dispersion pumping mechanism concurrently, can realize high average output power, the continuous spectrum output that high optical conversion efficiencies and spectral region are relatively wide.Be particularly suitable for application that average output power and spectral concentration are had relatively high expectations.This light source also utilizes ripe high power optical fibre laser technology, photonic crystal fiber manufacturing technology and photonic crystal fiber post-processing technology, has reduced system cost, is convenient to suitability for industrialized production and application.
Description of drawings
Fig. 1 is the structural representation of the super continuum source that proposes of the present invention.
Fig. 2 is the end face structure schematic diagram of the photonic crystal fiber of employing in specific embodiment one.
Embodiment
In figure: 1 pump laser for band output tail optical fiber; 2 is photonic crystal fiber; 3 for being with the output tail optical fiber of the pump laser of exporting tail optical fiber; 4 is fusion point; 5 is the base material of photonic crystal fiber; 6 is the fibre core of photonic crystal fiber; 7 is aperture.
The present invention is described in further detail below in conjunction with accompanying drawing and specific embodiment.Should be appreciated that specific embodiment described herein only is used for explaining the present invention, but should not limit protection scope of the present invention with this.
Fig. 1 is the structural representation based on the super continuum source of normal dispersion pumping 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, photonic crystal fiber 2, wherein, the output tail optical fiber 3 of the pump laser of band output tail optical fiber carries out welding with an end face of photonic crystal fiber 2 and consists of all optical fibre structure, fusion point 4.Pumping laser is coupled into photonic crystal fiber 2, due to the effect of various nonlinear effects, forms super continuous spectrums in photonic crystal fiber 2, and the super continuous spectrums of generation is from another end face output of photonic crystal fiber 2.
In specific embodiments of the invention one, pump laser 1 adopts the picopulse ytterbium-doping optical fiber laser, operation wavelength is near 1.06 microns, pulse duration is about 20 psecs, pulse repetition frequency is 500 megahertzes, average power is 56 watts, and output tail optical fiber 3 is 15 microns for core diameter, the doubly clad optical fiber that the inner cladding diameter is 130 microns; This pump laser is that basic mode distributes from the laser light field of tail optical fiber output.
Fig. 2 is the end face structure schematic diagram of the crystal fiber of employing in specific embodiment one.The base material 5 of this 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 end face, and be all the identical circular airport of bore dia, bore dia is 3.5 microns, the pitch of holes in two holes of arbitrary neighborhood is 5.4 microns, and fibre core is to form by an airport cancelling correspondence position.The zero dispersion point of this photonic crystal fiber is greatly near 1.11 microns, and 1.064 microns pumping lasers excite first order Raman Stokes peak is near 1.12 microns.In embodiment, the external diameter of photonic crystal fiber is vertically that optimizing length by analog computation is 3 m uniformly along optical fiber;
Under maximum pumping laser power, the super continuum source output average power based on the normal dispersion pumping of specific embodiment one is 50 W, and spectral region is the super continuous spectrums of 700-1700 nanometers, and optical conversion efficiencies reaches 90%.
Specific embodiment three is the Er-doped fiber laser of 1.5-1.6 micron left and right for pumping source adopts operation wavelength, and near the ZBLAN material of zero dispersion point 1.62 microns adopted in the substrate of photonic crystal fiber.
Specific embodiment four is mixing thulium or mixing the optical-fiber laser of holmium of 2 microns left and right for pumping source adopts operation wavelength, and near the SF57 material of zero dispersion point 2 microns adopted in the substrate of photonic crystal fiber.
Specific embodiment five is mixing thulium or mixing the optical-fiber laser of holmium of 2 microns left and right for pumping source adopts operation wavelength, and the base material of photonic crystal fiber adopts near the Bi material of zero dispersion point 2.29 microns.
Specific embodiment six is mixing thulium or mixing the optical-fiber laser of holmium of 2 microns left and right for pumping source adopts operation wavelength, and the base material of photonic crystal fiber adopts near the ZnTe material of zero dispersion point 2.24 microns.
Claims (9)
1. the super continuum source of a high-power high-efficiency, the pump laser, the photonic crystal fiber that comprise band output tail optical fiber, it is characterized in that, the output tail optical fiber of the pump laser of selecting is carried out welding with the input of photonic crystal fiber, namely consisted of the super continuum source of full fiberize;
Be specially: adopt the long pulse pumping laser to act on photonic crystal fiber normal dispersion district, the initial broadening of the leading spectrum of Raman scattering process; And make front what the centre wavelength at Raman Stokes peak that excites be positioned at the anomalous dispersion region near the zero dispersion point of photonic crystal fiber, before what is first or the second level, the Raman Stokes laser peak conduct that excites excites a new pumping source of super continuous spectrums, and satisfies the anomalous dispersion pumping mechanism; Fiber lengths is: the excited Raman effect can both effectively excite in the fiber lengths scope of use, and the energy that guarantees pumping laser can be transferred to Raman Stokes laser peak;
Described pump laser is: operation wavelength is positioned at the normal dispersion district of photonic crystal fiber, and when it acted on photonic crystal fiber, the centre wavelength at front what the Raman Stokes laser peak that excites was positioned at the anomalous dispersion region near the zero dispersion point of photonic crystal fiber; Pumping laser used is the long pulse pumping laser; Band tail optical fiber output, and the light beam of the laser of exporting from tail optical fiber is fundamental transverse mode or near fundamental transverse mode; Output of laser enters into photonic crystal fiber can excite super continuous spectrums effectively.
2. the super continuum source of a kind of high-power high-efficiency according to claim 1, it is characterized in that, pump laser is the rare-earth-doped fiber laser, rare earth ion comprises ytterbium, erbium, thulium, holmium, bismuth, be perhaps the fiber laser based on nonlinear effect, comprise Raman fiber lasers, parameteric light fibre laser; Being perhaps solid state laser, is perhaps semiconductor laser, by coupled system, Output of laser is coupled in optical fiber, consists of the pump laser of band output tail optical fiber.
3. the super continuum source of a kind of high-power high-efficiency according to claim 1, it is characterized in that, the end face of described photonic crystal is by the optical fiber base material, fibre core forms with the hole different from optical fiber base material refractive index, by changing refractive index, physical dimension and the arrangement mode of each several part, can realize different optic fibre characteristics.
4. the super continuum source of a kind of high-power high-efficiency according to claim 1, is characterized in that, the base material of described photonic crystal fiber can be pure quartz, can be also tellurides, sulfide or fluoride.
5. the super continuum source of a kind of high-power high-efficiency according to claim 1, it is characterized in that, the refractive index of the fibre core of described photonic crystal fiber can be identical with the optical fiber base material, also can be different, the refractive index of each fibre core and geometry can be identical, also can be different, can doped rare earth element in the material of fibre core, can not mix yet.
6. the super continuum source of a kind of high-power high-efficiency according to claim 1, it is characterized in that, the hole of described photonic crystal fiber end face can be airport, also can be filled by other high-index material, each hole can be the same with other hole, also can be different.
7. the super continuum source of a kind of high-power high-efficiency according to claim 1, is characterized in that, the external diameter of described photonic crystal fiber can be vertically uniformly along optical fiber, can be also non-homogeneous.
8. the super continuum source of a kind of high-power high-efficiency according to claim 1, it is characterized in that, when the output tail optical fiber of pump laser carries out welding with the input of photonic crystal fiber, can use the photonic crystal fiber post-processing technology, the photonic crystal fiber end face is processed, further reduced splice loss, splice attenuation.
9. the super continuum source of a kind of high-power high-efficiency according to claim 1, is characterized in that, described photonic crystal fiber has nonlinear characteristic, satisfies power condition and can produce the super continuous spectrums condition.
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Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103022867A (en) * | 2012-12-18 | 2013-04-03 | 中国人民解放军国防科学技术大学 | High-power high-efficiency supercontinuum source |
| CN104009377A (en) * | 2014-05-14 | 2014-08-27 | 北京工业大学 | Blue-light and ultraviolet-light enhancing super-continuum spectrum laser device of full-fiber structure |
| CN105449501A (en) * | 2015-12-29 | 2016-03-30 | 中国电子科技集团公司第十一研究所 | Fiber laser |
| CN107728403A (en) * | 2017-10-25 | 2018-02-23 | 中国地质大学（武汉） | A kind of 1.55 mu m waveband to 2 mu m wavebands wavelength shifter |
| CN113437629A (en) * | 2021-06-28 | 2021-09-24 | 中国科学院上海光学精密机械研究所 | Method for generating ultra-high relative intensity blue light supercontinuum |
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2012
- 2012-12-18 CN CN 201220702770 patent/CN203014156U/en not_active Expired - Fee Related
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103022867A (en) * | 2012-12-18 | 2013-04-03 | 中国人民解放军国防科学技术大学 | High-power high-efficiency supercontinuum source |
| CN104009377A (en) * | 2014-05-14 | 2014-08-27 | 北京工业大学 | Blue-light and ultraviolet-light enhancing super-continuum spectrum laser device of full-fiber structure |
| CN104009377B (en) * | 2014-05-14 | 2017-02-22 | 北京工业大学 | Blue-light and ultraviolet-light enhancing super-continuum spectrum laser device of full-fiber structure |
| CN105449501A (en) * | 2015-12-29 | 2016-03-30 | 中国电子科技集团公司第十一研究所 | Fiber laser |
| CN107728403A (en) * | 2017-10-25 | 2018-02-23 | 中国地质大学（武汉） | A kind of 1.55 mu m waveband to 2 mu m wavebands wavelength shifter |
| CN107728403B (en) * | 2017-10-25 | 2023-07-14 | 中国地质大学（武汉） | Wavelength converter with wavelength ranging from 1.55 mu m to 2 mu m |
| CN113437629A (en) * | 2021-06-28 | 2021-09-24 | 中国科学院上海光学精密机械研究所 | Method for generating ultra-high relative intensity blue light supercontinuum |
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