CN105870772A - Laser gain chip, laser assembly, power amplifier and oscillator - Google Patents
Laser gain chip, laser assembly, power amplifier and oscillator Download PDFInfo
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- CN105870772A CN105870772A CN201610430659.XA CN201610430659A CN105870772A CN 105870772 A CN105870772 A CN 105870772A CN 201610430659 A CN201610430659 A CN 201610430659A CN 105870772 A CN105870772 A CN 105870772A
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- laser
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- gain media
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/09—Processes or apparatus for excitation, e.g. pumping
- H01S3/091—Processes or apparatus for excitation, e.g. pumping using optical pumping
- H01S3/094—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
- H01S3/0941—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light of a laser diode
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/02—Constructional details
- H01S3/04—Arrangements for thermal management
- H01S3/042—Arrangements for thermal management for solid state lasers
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/14—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range characterised by the material used as the active medium
- H01S3/16—Solid materials
- H01S3/1601—Solid materials characterised by an active (lasing) ion
Abstract
The invention relates to a laser gain chip, a laser assembly, a power amplifier and an oscillator, and belongs to the technical field of laser equipment. The laser gain chip comprises a laser source, a gain medium, a pumping source and cooling fluid, wherein the pumping source comprises a diode array and a coupling device which are connected; the laser source, the coupling device and the cooling fluid are respectively arranged in a way of corresponding to different side surfaces of the gain media; the transmission directions of cooling fluid, pumping light and laser are in perpendicular quadrature; a gradual change doping structure is arranged inside the gain medium along the transmission direction of the pumping light. The three fields including the pumping field, the laser field and the cooling fluid field are in perpendicular quadrature; the space coupling in the three fields is relieved, so that each field can be independently controlled; in addition, each gain medium has a unique pumping source; a plurality of laser gain chips are in cascade connection in the laser transmission direction; the power expansion can be realized; the operation is convenient; the engineering implementation is facilitated.
Description
Technical field
The invention belongs to laser equipment technical field, relate in particular to a kind of laser gain chip and laser group
Part, power amplifier and agitator.
Background technology
High-average power laser has a wide range of applications in fields such as national defence, industry, scientific researches.High in repetition
Lath-shaped, laminated or flake gain media can be typically used with in device of high power laser.Lath
The advantage of shape medium is to constrain in inside lath by laser beam in the way of total reflection transmission, this transmission light
Road is referred to as in a zigzag (Zig-Zag) light path, and to have homogenized the optics of lath thickness direction uneven for light path in a zigzag
Property, reduce the thermal lensing effect thus caused and the birefringence effect caused by stress.Pumping schemes is by just
The laser diode-side-pumped of phase is developed to end-pumping, is improved to a centimetre amount from millimeter magnitude by the absorption length of pumping light
Level, it is ensured that the efficient absorption of pumping light, improves laser instrument aggregate efficiency.The lath of application light path in a zigzag
Solid state laser patent includes: 3,633,126;6,094,297;6,134,258 grades (U.S.).Laminated medium
Advantage to be laser transmit along interarea direction, and through interarea, owing to lamination interarea size is relatively big, Fresnel
Number is relatively big, thus is prone to multi-disc and realizes laser energy and power expansion along interarea direction stacking, and laser aid is tied
Structure is compact.The solid state laser patent of application laminated includes: US 7,366,211;CN 103650261 A
Deng.The advantage of sheet medium is that Laser Transmission direction is basically identical with conduction of heat direction, and thermograde exists
In laser propagation direction, each several part before laser wave experiences identical variations in temperature, thus, thermal distoftion is very
Little, it is ensured that higher beam quality.The solid state laser patent of application sheet medium includes: 3,631,362;
6,339,605 grades (U.S.).
Although lath-shaped, laminated or flake gain media have a lot of advantage, but, applying to weight
Frequently high energy and device of high power laser there is also deficiency.In lath-shaped laser aid, owing to need to ensure to dissipate
Heat energy power, causes medium thin, the laser chances of losing games be the end face of medium and bore little, be limited to diffraction loss with
Media size, the fan-out capability of monolithic lath is limited.Single-link merit is realized along medium length direction multi-disc stacking
During rate extension, it is difficult to ensure that the compact of laser aid, as patent is told 4,761,059 and 7,436,588 is (beautiful
State) use multilink Laser coherent combining to realize high-power output.Optics coherence tomography is spatially equivalent to increase
Laser beam size, owing to beam separation can not eliminate, causes far field beams power dissipation, and beam quality is not
Reach, be unfavorable for that it is applied.In laminated laser aid, pumping light and laser share the interarea of lamination,
The uniformity of pumping light field will directly affect the uniformity of laser near-field, want during multi-disc vertical stack power expansion
Seek higher pump intensity degree (such as 20kW/cm2), the several tens cm magnitude that diode array need to be sent
Light beam contracting bundle to centimetres, such as patent 5,307,430 and 6, what 160,934 (U.S.) used hollow leads
Pipe, its essence is a conical reflecting system, and laser beam compression necessarily causes the angle of divergence to increase, thus, contracting bundle
After the conformal transmission range of pumping light short, about at centimetres.Laminated laser power is limited to distribution all
Even, high intensity and the pumping light that can transmit.In flake laser aid, owing to the absorber thickness of thin slice exists
Hundred micron dimensions, one way is low to the absorption efficiency of pumping light.Patent 6,577,666 and 6,891,874 (U.S.)
Based on parabolic mirror the super many journeys pumping structure announced, utilizes this structure pumping light Multiple through then out thin slice
Efficient pumping can be realized, but this pumping structure is complicated.Thin slice typically use after interarea cooling mode, laser
Being exported after rear interarea reflects by front principal plane is incident, the light path of this amplification is referred to as " V " shape and amplifies light path.Adopt
Realizing power expansion by the mode of multiple amplifying head module-cascades, for making full use of pump field, intermodule uses
Image relaying system, the length dimension often increasing a module laser aid need to increase by four times of focal lengths, and tens of pieces thin
The laserresonator that sheet is constituted is up to 50 meters, and structure is complicated, bulky, it is more difficult to ensure the steady of laser aid
Qualitative.
Summary of the invention
For all deficiencies of prior art, in order to solve the problems referred to above, it is proposed that a kind of pump field, laser
Field, cooling three perpendicular laser gain chips of fluid field and laser module, power amplifier and vibration
Device, has gain and is uniformly distributed, is obtained in that higher beam quality, is prone to the feature of power expansion.
For achieving the above object, the present invention provides following technical scheme:
A kind of laser gain chip, including lasing light emitter, gain media, pumping source and cooling fluid, described pump
Source, Pu includes diode array and the coupling device being connected, described lasing light emitter, coupling device and cooling fluid
The not ipsilateral of the most corresponding gain media is arranged, and described cooling fluid, pump light, the transmission side of laser
Inside perpendicular quadrature, described gain media, the transmission direction along pump light is set to gradient doping structure.
Further, described gain media is set to laminated structure, and it includes center, mistake the most successively
Crossing layer and covering, described center and covering are disposed as gradient doping structure, and described transition zone is set to non-
Doped dielectric, the active ions of the internal doping in described center are Nd3+Or Yb3+, the internal correspondence of described covering is mixed
Miscellaneous active ions are Sm3+Or Cr4+, along the transmission direction of pump light, described center excited inside ion
Doping content is the Long-term change trend that low centre, two ends is high.
Further, the doping content of described center excited inside ion is:
By
Draw:
Wherein, ndRepresent the doping concentration distribution of center excited inside ion, ηPRepresent pump light absorption efficiency,
g0Represent small-signal gain, IPs,inRepresent the pumping light intensity that gain media both sides are total, I+ Ps,inRepresent gain media list
The pumping light intensity of side, and meetIPsRepresent the local pumping light intensity in gain media, I+ PsTable
Showing that single-side pumping light transmits direction distribution in gain media along it, described light intensity is pumping light intensity and pumping
The ratio of saturated light intensity, with the central point of center as zero, x represents the position along pumping optical transmission direction
Putting, W represents the center length along pumping optical transmission direction, σabsWith σemRepresent Pumping light absorption cross section respectively
With Laser emission cross section, A, B, C represent the hot population characteristic of dopant ion.
Further, described diode array includes symmetrically arranged diode array one centered by gain media
With diode array two, described diode array one and diode array two are respectively by coupling device and gain
Medium connects, and described coupling device is set to banded structure, and it is made up of multifiber, described coupling device
Height equal with the height of center, described pumping source sets at least to one, and adjacent coupled device is along it
Width arranges, and the overall width of coupling device is not more than the width of center.
Further, the side that described gain media is corresponding with lasing light emitter is coated with laser anti-reflection film, described laser
Transmit along the direction being perpendicular to described side, and through gain media, described coupling device sets with gain media
It is set to plane-plane contact, the side that described gain media contacts with coupling device is coated with pump light anti-reflection film, institute
State pump light internal along optic path in a zigzag at gain media.
Separately, the present invention also provides for a kind of laser module, including above-mentioned a kind of laser gain chip, described sharp
Gain of light chip is multiple along the cascade of Laser Transmission direction, and the spacing of adjacent laser chip gain is millimeter magnitude.
Separately, the present invention also provides for a kind of single laser cavity power amplifier, comprises above-mentioned a kind of laser gain core
Sheet, described laser gain chip cascades multiple composition laser modules, adjacent laser gain along Laser Transmission direction
The spacing of chip is millimeter magnitude, arranges front cavity mirror one and Effect of Back-Cavity Mirror one, described ante-chamber at described laser module
Mirror one, Effect of Back-Cavity Mirror one are total reflective mirror, are provided with quarter wave plate one at described Effect of Back-Cavity Mirror one.
Separately, the present invention also provides for a kind of bidifly optical cavity power amplifier, comprises above-mentioned a kind of laser gain core
Sheet, described laser gain chip separately constitutes laser module one and laser group along the cascade of Laser Transmission direction is multiple
Part two, the spacing of the adjacent laser chip gain being in same laser module is millimeter magnitude, described laser
90 ° of polarization apparatus rotors it are provided with between assembly one and laser module two.
Separately, the present invention also provides for a kind of agitator, includes front cavity mirror two, above-mentioned a kind of laser gain successively
Chip and Effect of Back-Cavity Mirror two, described laser gain chip cascades multiple composition laser modules along Laser Transmission direction,
The spacing of adjacent laser chip gain is millimeter magnitude, and described front cavity mirror two is set to total reflective mirror, described back cavity
Mirror two is set to partially reflecting mirror.
The invention has the beneficial effects as follows:
1, in the present invention, the not ipsilateral of lasing light emitter, coupling device and cooling fluid corresponding gain media respectively sets
Put, promote pump field, laser field and cooling three perpendicular quadratures of fluid field, relieve three couplings spatially
Close so that each field can independently control, beneficially engineering construction.
2, in the present invention, inside gain media, transmission direction along pump light is set to gradient doping structure, protects
In card gain media, gain is uniformly distributed, and this structure is highly suitable for quasi-three-level gain media or low suction
Receive the gain media of coefficient.
3, in the present invention, center and covering are disposed as gradient doping structure, and transition zone is set to undoped and is situated between
Matter, thus ensure that pump light is absorbed in center, transition zone effectively reduces the temperature ladder of center surrounding
Degree, reduces the depolarization loss caused by thermic stress birfringence, and covering can fully absorb spontaneous emission light,
Inhibit the self-oscillation that gain media is horizontal, it is ensured that the high-gain ability of gain media.
4, in the present invention, laser gain chip is multiple along the cascade of Laser Transmission direction, power expansion can be realized,
Each gain media is obtained in that in having independent pumping source, and each gain media that identical small-signal increases
Benefit, and gain profiles is uniform, pump energy and the heat production density of absorption have identical distribution, at power
In expansion process, it is not required to consider that other factors affect, simple operation, meanwhile, adjacent laser chip gain
Spacing is millimeter magnitude, and compact conformation takes up room little.
5, in the present invention, pump light is internal along optic path in a zigzag at gain media, has considerably long absorption
Length, the concentration adulterated by design is distributed, it can be ensured that high absorption efficiency and pumping homogeneity.
6, in the present invention, coupling device is formed by multifiber arrangement, when pumping source sets at least to one, many
Individual coupling device arranges along its width, is favorably improved pump power density, simultaneously as often
The output light field distribution of individual coupling device is identical, therefore, it is possible to while improving pump power, it is ensured that good
Good pumping homogeneity.
Accompanying drawing explanation
Fig. 1 is the overall structure schematic diagram of the present invention;
Fig. 2 be the present invention Fig. 1 in A-A cross-sectional view;
Fig. 3 be the present invention Fig. 1 in B-B cross-sectional view;
Fig. 4 is the gain medium structure schematic diagram of the present invention;
Fig. 5 is the coupling mechanism structure schematic diagram of the present invention;
Fig. 6 is the laser module plan structure schematic diagram of the present invention;
Fig. 7 is single laser cavity power amplifier structure schematic diagram of the present invention;
Fig. 8 is the bidifly optical cavity power amplifier structure schematic diagram of the present invention;
Fig. 9 is the oscillator structure schematic diagram of the present invention;
Figure 10 (a) is Nd in the embodiment of the present invention five3+The concentration distribution of ion linear doping and small-signal gain
Distribution relation figure;
B () is Nd in the embodiment of the present invention five3+The concentration distribution of ion gradient doping and small-signal gain
Distribution relation figure;
Figure 11 (a) is Yb in the embodiment of the present invention six3+The concentration distribution of ion linear doping and small-signal gain
Distribution relation figure;
B () is Yb in the embodiment of the present invention six3+The concentration distribution of ion gradient doping and small-signal gain
Distribution relation figure.
In accompanying drawing: 1-gain media, 101-center, 102-transition zone, 103-covering, 104-grow tall face, 105-
Wide high surface, 106-length and width face, 2-pumping source, 201-diode array one, 202-diode array two, 203-
Coupling device, 204-optical fiber, 3-laser, 4-pump light, 5-cool down fluid, 6-laser module shell, 61-window
Mouth, 62-housing, 7-fluid circulator, 8-fluid line, 9-lasing light emitter, 10-beam-expanding system one, 11-polarization
Sheet one, 12-45 ° of faraday, 13-45 ° of quartzy rotor, 14-polaroid two, 15-front cavity mirror one, 16-reflecting mirror
One, 17-reflecting mirror two, 18-Image relaying system one, 19-1/4 wave plate one, 20-Effect of Back-Cavity Mirror one, 21-reflecting mirror three,
22-beam-expanding system two, 23-reflecting mirror four, 24-polaroid three, 25-Image relaying system two, 26-1/4 wave plate two,
27-Image relaying system three, 28-90 ° of polarization apparatus rotor, 29-Image relaying system four, 30-reflecting mirror five, 31-electric light
Switch, 32-polaroid four, 33-reflecting mirror six, 34-laser module one, 35-laser module two, 36-front cavity mirror
Two, 37-Effect of Back-Cavity Mirror two.
In Figure 10, axis of abscissas represents the length of gain media, and unit is cm, and main axis of ordinates represents Nd3+
The doping concentration distribution of ion, unit is 1018/cm3, secondary axis of ordinates represents small-signal gain, and unit is cm-1,
Dotted line represents that small-signal gain, solid line represent Nd3+The doping concentration distribution of ion.
In Figure 11, axis of abscissas represents the length of gain media, and unit is cm, and main axis of ordinates represents Yb3+
The doping concentration distribution of ion, unit is 1019/cm3, secondary axis of ordinates represents small-signal gain, and unit is cm-1,
Dotted line represents that small-signal gain, solid line represent Yb3+The doping concentration distribution of ion.
Detailed description of the invention
In order to make those skilled in the art be more fully understood that technical scheme, attached below in conjunction with the present invention
Figure, carries out clear, complete description to technical scheme, based on the embodiment in the application, this
Other similar embodiment that field those of ordinary skill is obtained on the premise of not making creative work,
All should belong to the scope of the application protection.
Embodiment one:
As Figure 1-3, a kind of laser gain chip, including lasing light emitter, gain media 1, pumping source 2 and cold
But fluid 5, described pumping source 2 includes diode array and the coupling device 203 being connected, described diode battle array
Row include symmetrically arranged diode array 1 and diode array 1, institute centered by gain media 1
State diode array 1, diode array 1 to be connected with gain media 1 by coupling device 203 respectively,
Described coupling device 203 is set to banded structure, and it is formed by multifiber 204 arrangement, itself and gain media 1
It is set to plane-plane contact, utilizes the advantage of coupling device 203 flexible transfer, improve diode array and be situated between with gain
Matter 1 degree of freedom spatially, it is simple to pumping source 2 and gain media 1 are arranged, heat management.
Described lasing light emitter, coupling device 203 are arranged with the not ipsilateral of cooling fluid 5 corresponding gain media 1 respectively,
Promote pump field, laser field and cooling three perpendicular quadratures of fluid field, the transmission direction of the most described cooling fluid 5
With pump light 4, the transmission direction perpendicular quadrature of laser 3, relieve three couplings spatially so that each
Individual field all can independently control, beneficially engineering construction.
Being coated with laser anti-reflection film on the side that described gain media 1 is corresponding with lasing light emitter, described laser 3 is along vertically
Transmit in the direction of described side, and through gain media 1, described gain media 1 contacts with coupling device 203
Side on be coated with pump light anti-reflection film, promote described pump light 4 internal along light path in a zigzag at gain media 1
Transmission.
As preferably, described pump light 4 transmits, when the length of gain media 1 along the longest edge of gain media 1
During while be longest edge, described in grow tall and be coated with laser anti-reflection film on face 104, described wide high surface 105 is coated with pump light
Anti-reflection film, described laser 3 transmits along the direction, face of growing tall 104 being perpendicular to gain media 1, grows tall face 104 size relatively
Greatly, Fresnel number is relatively big, and described pump light 4 transmits along wide high surface 105 direction being perpendicular to gain media 1, promotees
Make between the pump light 4 face of growing tall 104 in gain media 1 along optic path in a zigzag, there is considerably long absorption
Length, is effectively increased absorption efficiency and pumping homogeneity, and described cooling fluid 5 is along being perpendicular to gain media 1
The transmission of direction, length and width face 106, the used heat in gain media 1 is taken away from the face of growing tall 104, there is efficient dissipating
Heat energy power, meanwhile, laser field is parallel with temperature gradient field, reduce gain media 1 thermal distoftion to laser wave before
Impact, it is ensured that beam quality.
Embodiment two:
As Figure 1-5, described gain media 1 is set to laminated structure, and along the biography of pump light 4 inside it
Defeated direction is set to gradient doping structure, it is ensured that the gain in gain media 1 is uniformly distributed, and this structure is very
Being applicable to quasi-three-level gain media or the gain media of low absorption coefficient, described gain media 1 is from inside to outside
Include that center 101, transition zone 102 and covering 103, described center 101 and covering 103 are disposed as successively
Gradient doping structure, the active ions of the internal doping in described center 101 are Nd3+Or Yb3+, thus ensure that
Pump light 4 is absorbed in center 101, and the active ions of the internal corresponding doping of described covering 103 are Sm3+Or
Cr4+, pump light 4 is absorbed few by it, high to laser 3 spontaneous radiation efficiency of light absorption, it is suppressed that gain media 1
Horizontal self-oscillation, it is ensured that the high-gain ability of gain media 1, described transition zone 102 is set to undoped
Medium, effectively reduces the thermograde of center 101 surrounding, reduces moving back caused by thermic stress birfringence
Loss partially, and along the transmission direction of pump light 4, the doping content of described center 101 excited inside ion is two
Holding the Long-term change trend that low centre is high, the doping content of described covering 103 excited inside ion is linearly or non-linear
Long-term change trend, described gain media 1 is set to mix the phosphate glass of Nd, it is possible to for crystal or pottery
Yb:YAG、Yb:CaF2、Nd:CaF2Or Nd:YAG.
The height of described coupling device 203 is equal with the height of center 101, and described pumping source 2 sets at least to
One, can further improve the gain ability of laser gain chip, adjacent coupled by increasing pumping source 2 quantity
Device 203 arranges along its width, and the overall width of coupling device 203 is not more than the width of center 101.
The present embodiment by 2 coupling devices 203 the most side by side, improves pump power density, single coupling
Locking device 203 is longitudinally formed by multifiber 204, and the width of single coupling device 203 is about 1mm.By
Output light field in each coupling device 203 is distributed identical, therefore, it is possible to while improving pump power,
Ensure good pumping homogeneity.
Embodiment three:
As a shown in Figure 6, a kind of laser module, comprise above-mentioned laser gain chip, described laser gain
Chip is multiple along the cascade of Laser Transmission direction, can realize power expansion, and each gain media 1 has independent
It is obtained in that identical small-signal gain in pumping source 2, and each gain media 1, and gain profiles is uniform,
The pump energy and the heat production density that absorb have identical distribution, during power expansion, are not required to consider
Other factors affect, and simple operation, meanwhile, the spacing of adjacent laser chip gain is millimeter magnitude, preferably
For 0.5-5mm, compact conformation, take up room little.
It is internal that described laser module is arranged on laser module shell 6, and described laser module shell 6 includes window 61
With housing 62, window 61 being coated with laser anti-reflection film, described laser is incident to laser module shell 6 through window 61
Inside, described housing 62 is set to light tight structure.Described laser module also includes fluid circulator 7 and fluid
Pipeline 8, described fluid circulator 7 is connected with housing 62 by fluid line 8, and described cooling fluid 5 is by fluid hose
Road 8 enters in laser module shell 6, flows through, taken away by heat between adjacent gain media 1.
Described cooling fluid 5 can use cooling liquid, and such as carbon tetrachloride, Carbon bisulfide, heavy water etc., gain is situated between
The Maximum pumping density that matter 1 the can bear boiling point with cooling liquid, the break limit phase of gain media 1
Closing, under the conditions of this, the spacing of adjacent laser chip gain is 0.5-3mm.Described cooling fluid 5 can use cold
But gas, such as helium etc., under the conditions of this, the spacing of adjacent laser chip gain is 2-5mm.
Embodiment four:
As it is shown in fig. 7, a kind of single laser cavity power amplifier, comprise above-mentioned laser gain chip, described sharp
Gain of light chip transmits direction along laser 3 and cascades multiple composition laser modules, the spacing of adjacent laser chip gain
For millimeter magnitude, preferably 0.5-5mm, along the transmission direction of laser 3, described amplifier includes same successively
The lasing light emitter 9 of optical axis setting, beam-expanding system 1, polaroid 12,45 ° of quartzy rotors of one 11,45 ° of faraday
13, polaroid 2 14, front cavity mirror 1, reflecting mirror 1, reflecting mirror 2 17, laser module, Image relaying system
Unification 18 and Effect of Back-Cavity Mirror 1, described front cavity mirror 1, Effect of Back-Cavity Mirror 1 are total reflective mirror, described Effect of Back-Cavity Mirror one
Quarter wave plate 1 it is provided with at 20.
Lasing light emitter 9 output laser 3, successively through beam-expanding system 1, one 11,45 ° of faraday 12 of polaroid,
After 45 ° of quartzy rotors 13, polaroid 2 14, reflecting mirror 1, reflecting mirrors 2 17, in injection laser module also
Pass perpendicularly through gain media 1, image in Effect of Back-Cavity Mirror 1 through Image relaying system 1, quarter wave plate 1,
Laser 3 realizes a Cheng Fang great, Effect of Back-Cavity Mirror 1 after the laser 3 returned sequentially passes through each element, through polaroid
2 14 reflex to front cavity mirror 1, and laser 3 realizes the second Cheng Fang great, front cavity mirror 1 laser 3 returned is again
Inject laser module, it is achieved three journeys, quadruple pass amplify, and repeat no more, after export through polaroid 1.
As shown in Figure 8, a kind of bidifly optical cavity power amplifier, comprise above-mentioned a kind of laser gain chip, institute
State laser gain chip to transmit direction cascade along laser 3 and multiple separately constitute laser module 1 and laser module two
35, the spacing of the adjacent laser chip gain being in same laser module is millimeter magnitude, is preferably
0.5-5mm。
Along the transmission direction of laser 3, described amplifier includes lasing light emitter 9, the reflection that same optical axis arranges successively
Mirror 3 21, beam-expanding system 2 22, reflecting mirror 4 23, polaroid 3 24, Image relaying system 2 25, quarter wave plate
2 26,3 27,90 ° of polarization apparatus rotors 28 of Image relaying system, Image relaying system 4 29, reflecting mirror 5 30, swash
Optical assembly 1, laser module 2 35, described reflecting mirror 3 21 and beam-expanding system 2 22 are set to off-axis out of focus knot
Structure, is provided with shielding system and reflecting mirror 6 33 at described polaroid 3 24, in time suppressing pumping from exciting
Swinging, it is ensured that the gain ability of system, described shielding system includes electrooptical switching 31, polaroid 4 32 successively.
The laser 3 of described lasing light emitter 9 output, the vertical paper of laser 3 polarization state, it is reflected mirror 3 21 successively, expands
After beam system 2 22, reflecting mirror 4 23, polaroid 3 24, Image relaying system 2 25, quarter wave plate 2 26, with
Circular polarization state injects in laser module 1, after 3 27,90 ° of polarization apparatus rotors 28 of Image relaying system, described
90 ° of polarization apparatus rotors 28 are used for compensating hot depolarization, are injected in laser module 2 35, through Image relaying system four
29, after reflecting mirror 5 30, again by laser module 2 35, laser module 1, after crossing quarter wave plate 2 26,
The polarization state of laser 3 is transformed into the polarization state of parallel paper by initial vertical paper polarization, is transmitted through polarization
Sheet 3 24, comes and goes through shielding system, reflecting mirror 6 33, and the polarization state of laser 3 keeps constant, and reflection light is again
Secondary through polaroid 3 24, laser 3 transmits with the polarization state of parallel paper, and transmitting procedure repeats no more, laser 3
After laser module 2 35, laser module 1, when crossing quarter wave plate 2 26, the polarization state of laser 3 returns to hang down
In straight paper, reflect from polaroid 3 24, be reflected mirror 4 23, beam-expanding system 2 22 output.
Described amplifier is applicable to impulse type bidifly optical cavity power amplifier, after removing shielding system, the suitableeest
For continuous bidifly optical cavity power amplifier.
As it is shown in figure 9, a kind of agitator, include front cavity mirror 2 36, above-mentioned a kind of laser gain chip successively
With Effect of Back-Cavity Mirror 2 37, it is multiple that described laser gain chip transmits direction cascade along laser 3, adjacent laser gain core
The spacing of sheet is millimeter magnitude, preferably 0.5-5mm, and described front cavity mirror 2 36 is set to total reflective mirror, described before
Chamber mirror 2 36 is it can also be provided that distorting lens, and to compensate wavefront distortion, it is anti-that described Effect of Back-Cavity Mirror 2 37 is set to part
Penetrate mirror.
Embodiment five:
As Figure 1-4, the present embodiment repeats no more, except for the difference that with the identical part of embodiment one, two:
Described gain media 1 is set to Nd:YAG, its a size of 120mm × 120mm × 10mm, center
101 bores are 100mm × 100mm, and transition zone 102 is pure YAG, and its overall width is 10mm, covering
The active ions of 103 internal doping are Sm3+, its overall width is 10mm, and described laser 3 is along being perpendicular to the face of growing tall
104 direction transmission, described pump light 4 is along being perpendicular to the transmission of wide high surface 105 direction, and described cooling fluid 5 is along vertically
Transmitting in direction, length and width face 106, described cooling fluid 5 is set to carbon tetrachloride liquid.
Along the transmission direction of pump light 4, the internal Nd in described center 1013+Doping content linearly trend become
Change, the internal Sm of described covering 1033+Doping content linearly Long-term change trend, pump light 4 power density is
330W/cm2, when absorption efficiency is 95%, Nd3+The concentration distribution of ion linear doping divides with small-signal gain
Cloth relation, as shown in Figure 10 (a), in figure, small signal gain coefficient transmits direction along pump light 4 is that center is low by two
The distribution that limit is high, gain profiles is uneven, is unfavorable for obtaining uniform laser near-field.
Along the transmission direction of pump light 4, the internal Nd in described center 1013+Doping content be two ends low in the middle of high
Long-term change trend, the internal Sm of described covering 1033+Doping content linearly Long-term change trend, described Nd3+Mix
Miscellaneous concentration is:
By
Draw:
Wherein, ndRepresent the doping concentration distribution of center 101 excited inside ion, ηPRepresent that pump light 4 absorbs
Efficiency, g0Represent small-signal gain, IPs,inRepresent the pumping light intensity that gain media 1 both sides are total, I+ Ps,inRepresent gain
The pumping light intensity of medium 1 one side, and meetIPsRepresent the local pumping light intensity in gain media,
I+ PsRepresent that single-side pumping light transmits direction distribution in gain media along it, described light intensity be pumping light intensity with
The ratio of pumping saturation light intensity, with the central point of center 101 as zero, x represents and transmits along pump light 4
The position in direction, W represents that the length in direction, σ are transmitted along pump light 4 in center 101absWith σemRepresent pump respectively
Pu light 4 absorption cross-section and Laser emission cross section, A, B, C represent the hot population characteristic of dopant ion.
Under room temperature, Nd3+Parameter is: σabs=6.7 × 10-20cm2, σem=28 × 10-20cm2, A=C=ηQ, B=0,
ηQ=1, wherein, ηQFor fluorescence efficiency, pump light 4 power density is 330W/cm2, ηP=95%, Nd3+From
Concentration distribution and the small signal gain distribution relation of sub-gradient doping, as shown in Figure 10 (b), along pumping in figure
Light 4 transmits direction and uses gradient doping, and concentration is distributed in class gaussian shaped profile, and the gain in gain media 1 divides
Cloth is uniform, and therefore, described laser gain chip is applicable to four-level system.
Embodiment six:
As Figure 1-4, the part that the present embodiment is identical with embodiment five repeats no more, except for the difference that:
Described gain media 1 is set to Yb:YAG, and the active ions of the internal doping of covering 103 are Cr4+, described
Cooling fluid 5 is set to helium.
Along the transmission direction of pump light 4, the internal Yb in described center 1013+Doping content linearly trend become
Change, the internal Cr of described covering 1034+Doping content be nonlinear trend change, pump light 4 power density is
9.4kW/cm2, when absorption efficiency is 95%, Yb3+The concentration distribution of ion linear doping divides with small-signal gain
Cloth relation, as shown in Figure 11 (a), in figure, small signal gain coefficient transmits direction along pump light 4 is that center is low by two
The distribution that limit is high, gain profiles is uneven, is unfavorable for obtaining uniform laser near-field.
Along the transmission direction of pump light 4, the internal Yb in described center 1013+Doping content be two ends low in
Between high Long-term change trend, the internal Cr of described covering 1034+Doping content be nonlinear trend change, at 200K
Time, Yb3+Parameter is: σabs=1.1 × 10-20cm2, σem=4.4 × 10-20cm2, f01=0.8749, f03=0.0464, f11=0.7667, f12=0.1846, wherein, fijRepresent pumping energy
The hot population ratio of level its residing multiplet shared with laser levels, pump light 4 power density is
9.4kW/cm2, ηP=95%, Yb3+Concentration distribution and the small signal gain distribution relation of ion gradient doping, as
Shown in Figure 11 (b), transmitting direction along pump light 4 and use gradient doping in figure, concentration is distributed in class Gaussian
Distribution, the gain profiles in gain media 1 is uniform, and therefore, described laser gain chip is applicable to accurate three energy
Level system.
Below the present invention is described in detail, the above, only the preferred embodiments of the invention,
When not limiting the scope of the present invention, the most all made impartial change according to the application scope and modified, all should be still
Belong in covering scope of the present invention.
Claims (9)
1. a laser gain chip, including lasing light emitter, gain media, pumping source and cooling fluid, described
Pumping source includes diode array and the coupling device being connected, it is characterised in that: described lasing light emitter, coupling
Device and the not ipsilateral setting of cooling fluid respectively corresponding gain media, and described cooling fluid, pump light,
The transmission direction perpendicular quadrature of laser, inside described gain media, the transmission direction along pump light is set to gradually
Varied doping structure.
A kind of laser gain chip the most according to claim 1, it is characterised in that: described gain media
Being set to laminated structure, it includes center, transition zone and covering the most successively, described center and
Covering is disposed as gradient doping structure, and described transition zone is set to undoped medium, inside described center
The active ions of doping are Nd3+Or Yb3+, the active ions of the internal corresponding doping of described covering are Sm3+Or Cr4+,
Along the transmission direction of pump light, the doping content of described center excited inside ion is that low centre, two ends is high
Long-term change trend.
A kind of laser gain chip the most according to claim 2, it is characterised in that: in described center
The doping content of portion's active ions is:
By
Draw:
Wherein, ndRepresent the doping concentration distribution of center excited inside ion, ηPRepresent pump light absorption efficiency,
g0Represent small-signal gain, IPs,inRepresent the pumping light intensity that gain media both sides are total, I+ Ps,inRepresent gain media list
The pumping light intensity of side, and meetIPsRepresent the local pumping light intensity in gain media, I+ PsTable
Showing that single-side pumping light transmits direction distribution in gain media along it, described light intensity is pumping light intensity and pumping
The ratio of saturated light intensity, with the central point of center as zero, x represents the position along pumping optical transmission direction
Putting, W represents the center length along pumping optical transmission direction, σabsWith σemRepresent Pumping light absorption cross section respectively
With Laser emission cross section, A, B, C represent the hot population characteristic of dopant ion.
A kind of laser gain chip the most according to claim 1, it is characterised in that: described diode battle array
Row include symmetrically arranged diode array one and diode array two centered by gain media, described two poles
Pipe array one and diode array two are connected with gain media by coupling device respectively, and described coupling device sets
Being set to banded structure, it is made up of multifiber, and the height of described coupling device is equal with the height of center,
Described pumping source sets at least to one, and adjacent coupled device arranges along its width, and coupling device
Overall width is not more than the width of center.
A kind of laser gain chip the most according to claim 1, it is characterised in that: described gain media
Being coated with laser anti-reflection film on the side corresponding with lasing light emitter, described laser passes along the direction being perpendicular to described side
Defeated, and through gain media, described coupling device and gain media are set to plane-plane contact, and described gain is situated between
Being coated with pump light anti-reflection film with coupling device on the side that matter contacts, described pump light is on the internal edge of gain media
Optic path in a zigzag.
6. a laser module, it is characterised in that: comprise the arbitrary described a kind of laser gain of claim 1-5
Chip, described laser gain chip is multiple along the cascade of Laser Transmission direction, the spacing of adjacent laser chip gain
For millimeter magnitude.
7. a single laser cavity power amplifier, it is characterised in that: comprise claim 1-5 arbitrary described one
Planting laser gain chip, described laser gain chip cascades multiple composition laser modules along Laser Transmission direction,
The spacing of adjacent laser chip gain is millimeter magnitude, arranges front cavity mirror one and Effect of Back-Cavity Mirror at described laser module
One, described front cavity mirror one, Effect of Back-Cavity Mirror one are total reflective mirror, are provided with quarter wave plate one at described Effect of Back-Cavity Mirror one.
8. a bidifly optical cavity power amplifier, it is characterised in that: comprise claim 1-5 arbitrary described one
Planting laser gain chip, described laser gain chip separately constitutes laser group along the cascade of Laser Transmission direction is multiple
Part one and laser module two, the spacing of the adjacent laser chip gain being in same laser module is millimeter amount
Level, is provided with 90 ° of polarization apparatus rotors between described laser module one and laser module two.
9. an agitator, it is characterised in that: include that front cavity mirror two, claim 1-5 are arbitrary described successively
A kind of laser gain chip and Effect of Back-Cavity Mirror two, described laser gain chip is multiple along the cascade of Laser Transmission direction,
The spacing of adjacent laser chip gain is millimeter magnitude, and described front cavity mirror two is set to total reflective mirror, described back cavity
Mirror two is set to partially reflecting mirror.
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CN117220122A (en) * | 2023-11-07 | 2023-12-12 | 中国工程物理研究院应用电子学研究所 | Plane waveguide laser gain module and laser amplifying device for 1.3um |
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