CN107290861A - Laser beam homogenization device and method - Google Patents

Laser beam homogenization device and method Download PDF

Info

Publication number
CN107290861A
CN107290861A CN201710645090.3A CN201710645090A CN107290861A CN 107290861 A CN107290861 A CN 107290861A CN 201710645090 A CN201710645090 A CN 201710645090A CN 107290861 A CN107290861 A CN 107290861A
Authority
CN
China
Prior art keywords
light
laser
prism
cylindrical mirror
diverging
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN201710645090.3A
Other languages
Chinese (zh)
Inventor
程根
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shenyang Zhuo Zhuo Laser Medical Instruments Co Ltd
Original Assignee
Shenyang Zhuo Zhuo Laser Medical Instruments Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shenyang Zhuo Zhuo Laser Medical Instruments Co Ltd filed Critical Shenyang Zhuo Zhuo Laser Medical Instruments Co Ltd
Priority to CN201710645090.3A priority Critical patent/CN107290861A/en
Publication of CN107290861A publication Critical patent/CN107290861A/en
Priority to PCT/CN2017/114221 priority patent/WO2019024359A1/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/09Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
    • G02B27/0927Systems for changing the beam intensity distribution, e.g. Gaussian to top-hat
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/09Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
    • G02B27/0938Using specific optical elements
    • G02B27/095Refractive optical elements
    • G02B27/0955Lenses
    • G02B27/0966Cylindrical lenses
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/09Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
    • G02B27/0938Using specific optical elements
    • G02B27/095Refractive optical elements
    • G02B27/0972Prisms

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Laser Beam Processing (AREA)
  • Lasers (AREA)

Abstract

The present invention proposes a kind of laser beam homogenization device and method, and for homogenizing the laser that power distribution is Gaussian Profile, the laser beam homogenization device includes:Diverging optical element group, for incident laser to be converted into diverging light;Beam splitter optic group, for being superimposed to form flat top beam to the diverging light beam splitting, and by the laser after beam splitting.By the laser beam homogenization device and method of the present invention, cost that the laser shaping that power distribution is Gaussian Profile is flat-top light is low, to wavelength without selectivity, rectangular light spot size is flexibly adjustable, also, is respectively provided with larger field depth and preferably homogenizes effect.

Description

Laser beam homogenization device and method
Technical field
The present invention relates to laser shaping field, more particularly to a kind of laser homogenizing device and method, by Laser beam energy distribution Gaussian Profile be converted into being uniformly distributed for flat roof type.
Background technology
The optical power distribution of laser cross-section is generally Gaussian Profile, i.e. center power greatly, more smaller to edge power.But It is in some application fields such as laser welding, Laser Surface Treatment and laser medicine, it is desirable to which the power distribution of laser is flat-top Being uniformly distributed for formula, you must use some optical shaping methods to realize the purpose.Flat-top light shaping side main at present Case has:Aperture diaphragm intercepts method, diffraction optical element method, microlens array shaping method, non-spherical lens method etc..Above shaping side Shortcoming is substantially, specific as follows in case implementation process:Aperture diaphragm method can realize simplest flat-top light output.But this method is obtained To homogenize effect not good, and optical energy loss is serious;Diffraction optical element method can only be designed targetedly according to demand, and one Denier, which changes the parameters such as optical maser wavelength, must just redesign, and the laser damage threshold of the program is relatively low, can be only applied to small work( Rate laser, and the design and manufacturing cost of diffraction optical element are higher, and assembly precision requires more harsh;Microlens array Shaping method cost is higher, region that is realizing is too small, easy product interference fringe shortcoming;Aspherical mirror in non-spherical lens method Cost of manufacture is equally higher.Therefore, the laser shaping scheme for needing a kind of with low cost and shaping effect good at present.
The content of the invention
In order to solve the above problems, the present invention proposes a kind of laser beam homogenization device and method, with provide it is a kind of into The good laser shaping scheme of this cheap and shaping effect.
In order to achieve the above object, laser beam homogenization device of the invention, for homogenizing power distribution for Gaussian Profile Laser, including:Diverging optical element group, for incident laser to be converted into diverging light;Beam splitter optic group, for pair Diverging light beam splitting, and the laser after beam splitting is superimposed to form flat top beam.
Further, diverging optical element group includes:First direction cylindrical mirror, for its incident light to be converted into first party Upward diverging light;Second direction cylindrical mirror, for its incident light to be converted to the diverging light in second direction;Light splitting optical member Part group includes:First direction prism, for its incident light on first direction beam splitting;Second direction prism, for entering to it Light is penetrated on second direction beam splitting;First direction is orthogonal with second direction;First direction cylindrical mirror, second direction cylindrical mirror, One direction prism, second direction prism are arranged in order along the light direction of propagation, and incident laser is injected by first direction cylindrical mirror, Second direction cylindrical mirror and first direction prism are passed sequentially through, is projected by second direction prism and forms flat top beam.
Further, diverging optical element group includes:First direction cylindrical mirror, for its incident light to be converted into first party Upward diverging light;Second direction cylindrical mirror, for its incident light to be converted to the diverging light in second direction;Light splitting optical member Part group includes:First direction prism, for its incident light on first direction beam splitting;Second direction prism, for entering to it Light is penetrated on second direction beam splitting;First direction is orthogonal with second direction;First direction cylindrical mirror, first direction prism, second Direction cylindrical mirror, second direction prism are arranged in order along the light direction of propagation, and incident laser is injected by first direction cylindrical mirror, First direction prism and second direction cylindrical mirror are passed sequentially through, is projected by second direction prism and forms flat top beam.
Further, diverging optical element group includes:First direction cylindrical mirror, for its incident light to be converted into first party Upward diverging light;Second direction cylindrical mirror, for its incident light to be converted to the diverging light in second direction;Light splitting optical member Part group includes:First direction prism, for its incident light on first direction beam splitting;Second direction prism, for entering to it Light is penetrated on second direction beam splitting;First direction is orthogonal with second direction;First direction cylindrical mirror, second direction cylindrical mirror, Two direction prisms, first direction prism are arranged in order along the light direction of propagation, and incident laser is injected by first direction cylindrical mirror, Second direction cylindrical mirror and second direction prism are passed sequentially through, is projected by first direction prism and forms flat top beam.
Further, diverging optical element group includes:First direction cylindrical mirror, for its incident light to be converted into first party Upward diverging light;Second direction cylindrical mirror, for its incident light to be converted to the diverging light in second direction;Light splitting optical member Part group includes:Two-way prism, for its incident light on first direction, second direction beam splitting;First direction and second direction It is orthogonal;First direction cylindrical mirror, second direction cylindrical mirror, two-way prism are arranged in order along the light direction of propagation, incident laser Injected by first direction cylindrical mirror, by second direction cylindrical mirror, projected by two-way prism and form flat top beam.
Further, diverging optical element group includes:Circular concavees lens, the diverging for its incident light to be converted to circle Light;Beam splitter optic group includes:Two-way prism, for its incident light on first direction, second direction beam splitting;First party To orthogonal with second direction;Circular concavees lens, two-way prism are arranged in order along the light direction of propagation, and incident laser is recessed by circle Lens are injected, and project to form flat top beam by two-way prism.
To achieve these goals, the invention also provides a kind of laser beam homogenizes method, for homogenizing power distribution For the laser of Gaussian Profile, including:Incident laser is converted into diverging light;To diverging light beam splitting, and by the laser after beam splitting Superposition forms flat top beam.
Further, incident laser is dissipated in a first direction, obtains first direction diverging light;First direction is dissipated Light dissipates in second direction, is converted into diverging light, first direction is orthogonal with second direction.
Further, to diverging light beam splitting, including:To diverging light on first direction beam splitting, the work(of the laser after beam splitting Rate distribution is symmetrical on first direction;To on the laser after first direction beam splitting on second direction beam splitting, swashing after beam splitting The power distribution of light is symmetrical on first and second direction, and first direction is orthogonal with second direction.
Further, the sum of the power of each point of the laser after beam splitting in the plane set is same value.
The beneficial effects of the present invention are by the laser beam homogenization device and method of the present invention, be by power distribution The laser shaping of Gaussian Profile is low for the cost of flat-top light, and to wavelength without selectivity, rectangular light spot size is flexibly adjustable, and And, it is respectively provided with larger field depth and preferably homogenizes effect.
Brief description of the drawings
In order to illustrate more clearly about the embodiment of the present invention or technical scheme of the prior art, below will be to embodiment or existing There is the accompanying drawing used required in technology description to be briefly described, it should be apparent that, drawings in the following description are only Some embodiments of the present invention, for those of ordinary skill in the art, without having to pay creative labor, also Other accompanying drawings can be obtained according to these accompanying drawings.
Figure 1A is the structure and light path schematic diagram of the laser beam homogenization device of the embodiment of the present invention.
Figure 1B is the power distribution schematic diagram of the incident light of the embodiment of the present invention.
Fig. 1 C are the power distribution schematic diagram of the emergent light of the embodiment of the present invention.
Fig. 2 is the structural representation of the laser beam homogenization device of second embodiment of the invention.
Fig. 3 A are the structural representation of the laser beam homogenization device of third embodiment of the invention.
Fig. 3 B are the power profile of the incident light of third embodiment of the invention.
Fig. 3 C are the power profile of the emergent light of third embodiment of the invention.
Fig. 3 D are the power profile of the emergent light that the second cylinder curvature radius is 12mm in third embodiment of the invention.
Fig. 4 is the structural representation of the laser beam homogenization device of fourth embodiment of the invention.
Fig. 5 is the structural representation of the laser beam homogenization device of fifth embodiment of the invention.
Fig. 6 is the structural representation of the laser beam homogenization device of sixth embodiment of the invention.
Fig. 7 homogenizes the step flow chart of method for the laser beam of the embodiment of the present invention.
Embodiment
Below in conjunction with the accompanying drawing in the embodiment of the present invention, the technical scheme in the embodiment of the present invention is carried out clear, complete Site preparation is described, it is clear that described embodiment is only a part of embodiment of the invention, rather than whole embodiments.Based on this Embodiment in invention, the every other reality that relevant technical staff in the field is obtained under the premise of creative work is not made Example is applied, the scope of the protection of the present invention is belonged to.
Figure 1A is the structure and light path schematic diagram of the laser beam homogenization device of the embodiment of the present invention.As shown in Figure 1A, swash Light process for light beam homogenization device, for homogenizing the laser that power distribution is Gaussian Profile, including:Diverging optical element group 100, for inciting somebody to action Incident laser is converted to diverging light;Beam splitter optic group 200, for diverging light beam splitting, and by the laser stacking after beam splitting Plus form flat top beam.
Figure 1B is the power distribution schematic diagram of the incident light of the embodiment of the present invention, and Fig. 1 C are the emergent light of the embodiment of the present invention Power distribution schematic diagram.With reference to shown in Figure 1A, Figure 1B and Fig. 1 C, incident light is the laser that power distribution is Gaussian Profile, its It is in divergent state, the Energy distribution of the output light (diverging light) of the diverging optical element 100 after diverging optical element group 100 It is centrosymmetric, to be convenient to follow-up input operation.Beam splitter optic group 200, its input light is diverging optical element 100 Output light (diverging light), 200 points by beam splitter optic group of the diverging light is multiple laser, the Energy distribution phase of the multiple laser Mutually symmetrical, the multiple laser after beam splitting continues to propagate forward, and common irradiation is on a setting face, and the multiple laser energy is mutually folded Plus (be overlapped mutually and represented with the quadrangle of the different twill fillings of two beams in Figure 1A), eventually form flat top beam.It is described herein It is that what Figure 1A only illustrated is illustrated in the power distribution state of the input light and output light in one direction, those skilled in the art should It is respectively Gaussian Profile with being uniformly distributed when understanding input light with exporting photophase distribution spatially.
Fig. 2 is the structural representation of the laser beam homogenization device of second embodiment of the invention.As shown in Fig. 2 laser light In beam homogenizer, diverging optical element group includes:First direction cylindrical mirror 110, for its incident light to be converted into first party Upward diverging light;Second direction cylindrical mirror 120, for its incident light to be converted to the diverging light in second direction;Beam splitting light Learning element group includes:First direction prism 210, for its incident light on first direction beam splitting;Second direction prism 220, For to its incident light on second direction beam splitting;First direction is orthogonal with second direction;First direction cylindrical mirror 110, second Direction cylindrical mirror 120, first direction prism 210, second direction prism 220 are arranged in order along the light direction of propagation, and incident swashs Light is entered by the mirror of first direction cylinder 110, second direction cylindrical mirror 120 and first direction prism 210 is passed sequentially through, by second Direction prism 220 projects and forms flat top beam.
Incident light is the laser that power distribution is Gaussian Profile, its first direction cylinder passed through in diverging optical element group After mirror 110, the incident light is converted to the diverging light on first direction, and then the divergent light input on the first direction is to second party To cylindrical mirror 120, it continues to be converted to the diverging light in second direction, so far, the output light of second direction cylindrical mirror 120 on First direction is symmetrical with second direction.Again because first direction is perpendicular to second direction, that is to say, that the energy of the diverging light point Cloth is centrosymmetric.Then, the diverging light continues through first direction prism 210, is divided into two beams symmetrical on first direction Laser, the two beams laser again by second direction prism 220, its per it is a branch of all by second direction prism 220 points be that two beams are closed In the symmetrical laser of second direction.Exported finally by second direction prism on first direction and second direction respectively symmetrically Four beam laser.Due to the output light power distribution on first direction and second direction respectively symmetrically, so propagating one section After distance, common irradiation is on the face of a setpoint distance, and its power is overlapped mutually to form flat top beam.
Fig. 3 A are the structural representation of the laser beam homogenization device of third embodiment of the invention.As shown in Figure 3A, laser In process for light beam homogenization device, diverging optical element group includes:First direction cylindrical mirror 110, for its incident light to be converted into first Diverging light on direction;Second direction cylindrical mirror 120, for its incident light to be converted to the diverging light in second direction;Beam splitting Optical element group includes:First direction prism 210, for its incident light on first direction beam splitting;Second direction prism 220, for its incident light on second direction beam splitting;First direction is orthogonal with second direction;First direction cylindrical mirror 110, First direction prism 210, second direction cylindrical mirror 120, second direction prism 220 are arranged in order along the light direction of propagation, incident Laser entered by the mirror of first direction cylinder 110, pass sequentially through first direction prism 210 and second direction cylindrical mirror 120, by Second direction prism 220 projects and forms flat top beam.
Incident light is the laser that power distribution is Gaussian Profile, its first direction cylinder passed through in diverging optical element group After mirror 110, the incident light is converted to the diverging light output on first direction, according to the direction of propagation of light, on the first direction Divergent light input is to first direction prism 210, and the diverging light on first direction divide into two beams on first direction.Two beam Laser continues to propagate forward, by second direction cylindrical mirror 120, and the two beams laser is converted into while in a first direction with second Diverging light on direction.Finally, by second direction prism 220 export on first direction and second direction respectively symmetrically four Shu Jiguang.Due to the output light power distribution on first direction and second direction respectively symmetrically, so propagate one section away from From rear, common irradiation is on the face of a setpoint distance, and its power is overlapped mutually to form flat top beam.
It is assumed that LASER Light Source position be origin, incident light spot energy distribution as shown in Figure 3 B, apart from origin 70mm~ The rectangle flat-top hot spot that size is 50X20mm is obtained at 90mm, the angle of divergence is 18 °~22 ° (full-shape), and the correlation of the present embodiment is thoroughly Mirror parameter combination can make following selection:
First direction cylindrical mirror:Plano-concave cylindrical mirror, plane uses K9 glass, thick 1.5mm~2.5mm, concave surface towards light source Place's radius of curvature is 15mm~25mm, with initial point distance 8mm~12mm;
First direction prism:Plane is towards light source, using K9 glass, thick 2mm~4mm, and the angle between two inclined-planes is 20 °~35 °, with initial point distance 10mm~16mm;
Second direction cylindrical mirror:Concave-concave cylindrical mirror, using K9 glass, thick 1.8mm~2.2mm, the radius of curvature of concave surface is 10mm~10.8mm, is 16.9mm~17.9mm with initial point distance;
Second direction prism:Plane is towards light source, using K9 glass, thick 5mm~8mm, and the angle between two inclined-planes is 105 °~115 °, with initial point distance 20mm~23mm.
According to one group of specific lens parameter of said lens parameter group conjunction, spot energy distribution as shown in Figure 3 C, can be seen Go out target spot energy distribution uniform, according to the second direction cylindrical mirror that radius of curvature is 12mm, other lenses parameter constant, Its spot energy distribution is as shown in Figure 3 D, it can be seen that target spot energy distribution is high in the low surrounding in center, not flat top beam.
Fig. 4 is the structural representation of the laser beam homogenization device of fourth embodiment of the invention.As shown in figure 4, laser light In beam homogenizer, diverging optical element group includes:First direction cylindrical mirror 110, for its incident light to be converted into first party Upward diverging light;Second direction cylindrical mirror 120, for its incident light to be converted to the diverging light in second direction;Beam splitting light Learning element group includes:First direction prism 210, for its incident light on first direction beam splitting;Second direction prism 220, For to its incident light on second direction beam splitting;First direction is orthogonal with second direction;First direction cylindrical mirror 110, second Direction cylindrical mirror 120, second direction prism 220, first direction prism 210 are arranged in order along the light direction of propagation, and incident swashs Light is entered by the mirror of first direction cylinder 110, second direction cylindrical mirror 120 and second direction prism 220 is passed sequentially through, by first Direction prism 210 projects and forms flat top beam.
Incident light is the laser that power distribution is Gaussian Profile, its first direction cylinder passed through in diverging optical element group After mirror 110, the incident light is converted to the diverging light on first direction, and then the divergent light input on the first direction is to second party To cylindrical mirror 120, it continues to be converted to the diverging light in second direction, so far, the output light of second direction cylindrical mirror 120 on First direction is symmetrical with second direction.Again because first direction is perpendicular to second direction, that is to say, that the energy of the diverging light point Cloth is centrosymmetric.Then, the diverging light continues through second direction prism 220, is divided into two beams symmetrical on second direction Laser, the two beams laser again by first direction prism 210, its per it is a branch of all by first direction prism 210 points be that two beams are closed In the symmetrical laser of second direction, export right respectively on first direction and second direction finally by first direction prism 210 The four beam laser claimed.Due to the output light power distribution on first direction and second direction respectively symmetrically, so propagating After one segment distance, common irradiation is on the face of a setpoint distance, and its power is overlapped mutually to form flat top beam.
The structural representation of the laser beam homogenization device of Fig. 5 fifth embodiment of the invention.As shown in figure 5, laser beam In homogenizer, diverging optical element group includes:First direction cylindrical mirror 110, for its incident light to be converted into first direction On diverging light;Second direction cylindrical mirror 120, for its incident light to be converted to the diverging light in second direction;Light splitting optical Element group includes:Two-way prism 230, for its incident light on first direction, second direction beam splitting;First direction and second Direction is orthogonal;First direction cylindrical mirror 110, second direction cylindrical mirror 120, two-way prism 230 are arranged successively along the light direction of propagation Row, incident laser is entered by the mirror of first direction cylinder 110, by second direction cylindrical mirror 120, projected by two-way prism 230 Form flat top beam.In the 5th embodiment, and unlike first embodiment, the beam splitter optic is two-way prism 230, Incident light can be split by the two-way prism 230, and the laser after beam splitting is symmetrical with second direction on first direction.Due to The power distribution of the output light on first direction and second direction respectively symmetrically, it is common to shine so after a segment distance is propagated Penetrate on the face in a setpoint distance, its power is overlapped mutually to form flat top beam.
The structural representation of the laser beam homogenization device of Fig. 6 sixth embodiment of the invention.As shown in fig. 6, laser beam In homogenizer, diverging optical element group includes:Circular concavees lens 130, the diverging light for its incident light to be converted to circle; Beam splitter optic group includes:Two-way prism 230, for its incident light on first direction, second direction beam splitting;First party To orthogonal with second direction;Concavees lens 130, two-way prism 230 are arranged in order along the light direction of propagation.In the sixth embodiment, From unlike the 5th embodiment, the diverging optical element group is circular concavees lens 130, the circular concavees lens, the lens can be with Incident light is converted to the centrosymmetric diverging light of circle.Because the power distribution of the output light is on first direction and second party To respectively symmetrically, so after a segment distance is propagated, common irradiation is on the face of a setpoint distance, and its power is overlapped mutually to be formed Flat top beam.
The laser beam homogenization device of the present invention can be adjusted according to target light spot shape and dissipated in specific implementation process Optical element group and beam splitter optic group.If target is the flat top beam of regular hexagon, diverging optical element group includes:First Direction cylindrical mirror, for its incident light to be converted to the diverging light on first direction;Second direction cylindrical mirror, for it is incident Light is converted to the diverging light in second direction;Third direction cylindrical mirror, for its incident light to be converted to the hair on third direction Astigmatism;Beam splitter optic group includes:First direction prism, for its incident light on first direction beam splitting;Second direction Prism, for its incident light on second direction beam splitting;Third direction prism, for dividing on third direction its incident light Beam;The angle of first direction, second direction, third direction arbitrarily between the two is 120 °;First direction cylindrical mirror, second direction Cylindrical mirror, third direction cylindrical mirror first direction prism, second direction prism, third direction prism along the light direction of propagation successively Arrange, or other are various, the prism arrangement on certain direction can be met in the arrangement mode after equidirectional cylindrical mirror It is required that.Those skilled in the art can be according to embodiments of the present invention, by adjusting diverging optical element group and beam splitter optic The optical element combination of group, obtains target hot spot of different shapes, will not enumerate herein.
With reference to shown in above example, the advantage of laser beam homogenization device of the invention is as follows:
1. the cost degradation of flat-top light shaping can be realized.Because either cylindrical mirror, circular concavees lens or prism, all Being at present can be cheap and be easy to get by producing obtained universal optical element in batches.
2. the laser beam homogenization device of the present invention is to wavelength without selectivity.Cylindrical mirror and prism can pass through optics Glass system is obtained, in the wave-length coverage that optical glass can be passed through, and the device is applicable.
3. laser damage threshold is high, optical energy loss is low.Due to the internal opticses member of the laser beam homogenization device of the present invention Part can use optical glass to make, so laser damage threshold is high, optical energy loss is low.Optical glass has very high energy Damage threshold and optical transmittance, by plating optical film on its surface, it is possible to realize very high laser transmittance.
4. rectangular light spot size is big and adjustable.Because the light beam of generation is diverging light, as long as by reasonably changing prism Angle and lens radius of curvature, we can be obtained by the uniform rectangular light beam of the given size on predetermined distance.
Preferably effect is homogenized 5. being respectively provided with larger field depth.And diffraction optical element method, microlens array shaping Method, non-spherical lens method can only typically have preferable laser homogenizing effect in the face of being designed like, once imaging surface is movable, Effect is then homogenized to decline rapidly.
After the laser beam homogenization device of the embodiment of the present invention is described, next, swashing to the embodiment of the present invention Light beam homogenization method is introduced.The implementation of this method may refer to the implementation of said apparatus, repeats part and repeats no more.
Fig. 7 homogenizes the step flow chart of method for the laser beam of the embodiment of the present invention.As shown in fig. 7, laser-beam uniform-light Change method, for homogenizing the laser that power distribution is Gaussian Profile, including:S100, diverging light is converted to by incident laser; S200, is superimposed to form flat top beam to diverging light beam splitting, and by the laser after beam splitting.
During specific implementation step S100, incident laser is converted into diverging light, including:
S110, incident laser is dissipated in a first direction, obtains first direction diverging light;
S120, first direction diverging light is dissipated in second direction, diverging light, first direction and second party is converted into To orthogonal.
During specific implementation step S200, to diverging light beam splitting, including:
S210, to diverging light on first direction beam splitting, the power distribution of the laser after beam splitting is symmetrical on first direction;
S220, to, on second direction beam splitting, the power of the laser after beam splitting divides on the laser after first direction beam splitting Cloth is symmetrical on first and second direction, and first direction is orthogonal with second direction.
The sum of the power of each point of the laser in the plane set after beam splitting is same value.
The beneficial effects of the present invention are by the laser beam homogenization device and method of the present invention, be by power distribution The laser shaping of Gaussian Profile is low for the cost of flat-top light, and to wavelength without selectivity, rectangular light spot size is flexibly adjustable, and It is respectively provided with larger field depth and preferably homogenizes effect.
Above-described embodiment, has been carried out further to the purpose of the present invention, technical scheme and beneficial effect Describe in detail, should be understood that the embodiment that the foregoing is only the present invention, be not intended to limit the present invention Protection domain, within the spirit and principles of the invention, any modification, equivalent substitution and improvements done etc. all should be included Within protection scope of the present invention.

Claims (10)

1. a kind of laser beam homogenization device, for homogenizing the laser that power distribution is Gaussian Profile, it is characterised in that including:
Diverging optical element group, for incident laser to be converted into diverging light;
Beam splitter optic group, for being superimposed to form flat top beam to the diverging light beam splitting, and by the laser after beam splitting.
2. laser beam homogenization device according to claim 1, it is characterised in that
The diverging optical element group includes:
First direction cylindrical mirror, for its incident light to be converted to the diverging light on first direction;
Second direction cylindrical mirror, for its incident light to be converted to the diverging light in second direction;
The beam splitter optic group includes:
First direction prism, for its incident light on the first direction beam splitting;
Second direction prism, for its incident light on the second direction beam splitting;
The first direction is orthogonal with second direction;
The first direction cylindrical mirror, second direction cylindrical mirror, first direction prism, second direction prism are along the light direction of propagation Be arranged in order, the incident laser is injected by the first direction cylindrical mirror, pass sequentially through the second direction cylindrical mirror with And first direction prism, projected by the second direction prism and form flat top beam.
3. laser beam homogenization device according to claim 1, it is characterised in that
The diverging optical element group includes:
First direction cylindrical mirror, for its incident light to be converted to the diverging light on first direction;
Second direction cylindrical mirror, for its incident light to be converted to the diverging light in second direction;
The beam splitter optic group includes:
First direction prism, for its incident light on the first direction beam splitting;
Second direction prism, for its incident light on the second direction beam splitting;
The first direction is orthogonal with second direction;
The first direction cylindrical mirror, first direction prism, second direction cylindrical mirror, second direction prism are along the light direction of propagation Be arranged in order, the incident laser is injected by the first direction cylindrical mirror, pass sequentially through the first direction prism and Second direction cylindrical mirror, is projected by the second direction prism and forms flat top beam.
4. laser beam homogenization device according to claim 1, it is characterised in that
The diverging optical element group includes:
First direction cylindrical mirror, for its incident light to be converted to the diverging light on first direction;
Second direction cylindrical mirror, for its incident light to be converted to the diverging light in second direction;
The beam splitter optic group includes:
First direction prism, for its incident light on the first direction beam splitting;
Second direction prism, for its incident light on the second direction beam splitting;
The first direction is orthogonal with second direction;
The first direction cylindrical mirror, second direction cylindrical mirror, second direction prism, first direction prism are along the light direction of propagation Be arranged in order, the incident laser is injected by the first direction cylindrical mirror, pass sequentially through the second direction cylindrical mirror with And second direction prism, projected by the first direction prism and form flat top beam.
5. laser beam homogenization device according to claim 1, it is characterised in that
The diverging optical element group includes:
First direction cylindrical mirror, for its incident light to be converted to the diverging light on first direction;
Second direction cylindrical mirror, for its incident light to be converted to the diverging light in second direction;
The beam splitter optic group includes:
Two-way prism, for its incident light on the first direction, second direction beam splitting;
The first direction is orthogonal with second direction;
The first direction cylindrical mirror, second direction cylindrical mirror, two-way prism are arranged in order along the light direction of propagation, the incidence Laser injected by the first direction cylindrical mirror, by the second direction cylindrical mirror, projected and formed by the two-way prism Flat top beam.
6. laser beam homogenization device according to claim 1, it is characterised in that
The diverging optical element group includes:
Circular concavees lens, the diverging light for its incident light to be converted to circle;
The beam splitter optic group includes:
Two-way prism, for its incident light on first direction, second direction beam splitting;
The first direction is orthogonal with second direction;
The circular concavees lens, two-way prism are arranged in order along the light direction of propagation, and the incident laser is recessed by the circle Lens are injected, and project to form flat top beam by the two-way prism.
7. a kind of laser beam homogenizes method, for homogenizing the laser that power distribution is Gaussian Profile, it is characterised in that including:
The incident laser is converted into diverging light;
It is superimposed to form flat top beam to the diverging light beam splitting, and by the laser after beam splitting.
8. laser beam according to claim 7 homogenizes method, it is characterised in that described to change the incident laser For diverging light, including:
The incident laser is dissipated in a first direction, first direction diverging light is obtained;
The first direction diverging light is dissipated in second direction, the diverging light is converted into, the first direction and the Two directions are orthogonal.
9. laser beam according to claim 7 homogenizes method, it is characterised in that described to the diverging light beam splitting, bag Include:
To the diverging light on first direction beam splitting, the power distribution of the laser after beam splitting is symmetrical on first direction;
To the laser after the beam splitting on first direction on second direction beam splitting, the power distribution of the laser after beam splitting on The first direction is symmetrical with second direction, and the first direction is orthogonal with second direction.
10. laser beam according to claim 7 homogenizes method, it is characterised in that the laser after the beam splitting is in setting Plane on each point power sum be same value.
CN201710645090.3A 2017-08-01 2017-08-01 Laser beam homogenization device and method Pending CN107290861A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
CN201710645090.3A CN107290861A (en) 2017-08-01 2017-08-01 Laser beam homogenization device and method
PCT/CN2017/114221 WO2019024359A1 (en) 2017-08-01 2017-12-01 Laser beam homogenizing device and method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710645090.3A CN107290861A (en) 2017-08-01 2017-08-01 Laser beam homogenization device and method

Publications (1)

Publication Number Publication Date
CN107290861A true CN107290861A (en) 2017-10-24

Family

ID=60104541

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710645090.3A Pending CN107290861A (en) 2017-08-01 2017-08-01 Laser beam homogenization device and method

Country Status (2)

Country Link
CN (1) CN107290861A (en)
WO (1) WO2019024359A1 (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2019024359A1 (en) * 2017-08-01 2019-02-07 沈阳雷卓激光医疗器械有限公司 Laser beam homogenizing device and method
CN110993741A (en) * 2019-12-20 2020-04-10 武汉帝尔激光科技股份有限公司 Multi-pulse homogenization laser solar cell processing method and equipment
CN111258076A (en) * 2018-11-30 2020-06-09 福州高意光学有限公司 Optical system capable of realizing laser beam homogenization function
CN112987476A (en) * 2021-03-08 2021-06-18 中国科学院重庆绿色智能技术研究院 Holographic speckle screen for projection display system
CN115113409A (en) * 2022-08-26 2022-09-27 成都莱普科技股份有限公司 Linear flat-top light spot generation system, method and equipment based on Dammann grating
CN116931286A (en) * 2023-09-15 2023-10-24 成都莱普科技股份有限公司 Beam shaping module, method and device

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114967001A (en) * 2022-05-20 2022-08-30 武汉镭健科技有限责任公司 Rectangular light spot coupler

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4149773A (en) * 1975-12-23 1979-04-17 Plessey Handel Und Investments A.G. Optical system for the production of a beam of light having a uniform intensity distribution
US4370026A (en) * 1979-09-10 1983-01-25 Thomson-Csf Illuminating device for providing an illumination beam with adjustable distribution of intensity and a pattern-transfer system comprising such a device
US4523809A (en) * 1983-08-04 1985-06-18 The United States Of America As Represented By The Secretary Of The Air Force Method and apparatus for generating a structured light beam array
GB2220502A (en) * 1988-07-09 1990-01-10 Exitech Ltd Excimer laser beam homogenizer system
US5548444A (en) * 1994-07-06 1996-08-20 Hughes Danbury Optical Systems, Inc. Optical beam homogenizing apparatus and method
US6380966B1 (en) * 1999-01-29 2002-04-30 Fuji Photo Film Co., Ltd. Exposure recording device for scanning a recording medium with a light beam
US20030173503A1 (en) * 2002-03-14 2003-09-18 Science & Engineering Associates, Inc. Multiple imaging system and method for designing same
CN207181837U (en) * 2017-08-01 2018-04-03 沈阳雷卓激光医疗器械有限公司 Laser beam homogenization device

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102937746B (en) * 2012-10-30 2015-01-28 泉州师范学院 Long-distance generating system of approximate diffraction-free grating line structured lights
CN107290861A (en) * 2017-08-01 2017-10-24 沈阳雷卓激光医疗器械有限公司 Laser beam homogenization device and method

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4149773A (en) * 1975-12-23 1979-04-17 Plessey Handel Und Investments A.G. Optical system for the production of a beam of light having a uniform intensity distribution
US4370026A (en) * 1979-09-10 1983-01-25 Thomson-Csf Illuminating device for providing an illumination beam with adjustable distribution of intensity and a pattern-transfer system comprising such a device
US4523809A (en) * 1983-08-04 1985-06-18 The United States Of America As Represented By The Secretary Of The Air Force Method and apparatus for generating a structured light beam array
GB2220502A (en) * 1988-07-09 1990-01-10 Exitech Ltd Excimer laser beam homogenizer system
US5548444A (en) * 1994-07-06 1996-08-20 Hughes Danbury Optical Systems, Inc. Optical beam homogenizing apparatus and method
US6380966B1 (en) * 1999-01-29 2002-04-30 Fuji Photo Film Co., Ltd. Exposure recording device for scanning a recording medium with a light beam
US20030173503A1 (en) * 2002-03-14 2003-09-18 Science & Engineering Associates, Inc. Multiple imaging system and method for designing same
CN207181837U (en) * 2017-08-01 2018-04-03 沈阳雷卓激光医疗器械有限公司 Laser beam homogenization device

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2019024359A1 (en) * 2017-08-01 2019-02-07 沈阳雷卓激光医疗器械有限公司 Laser beam homogenizing device and method
CN111258076A (en) * 2018-11-30 2020-06-09 福州高意光学有限公司 Optical system capable of realizing laser beam homogenization function
CN110993741A (en) * 2019-12-20 2020-04-10 武汉帝尔激光科技股份有限公司 Multi-pulse homogenization laser solar cell processing method and equipment
CN112987476A (en) * 2021-03-08 2021-06-18 中国科学院重庆绿色智能技术研究院 Holographic speckle screen for projection display system
CN112987476B (en) * 2021-03-08 2022-07-29 中国科学院重庆绿色智能技术研究院 Holographic speckle screen for projection display system
CN115113409A (en) * 2022-08-26 2022-09-27 成都莱普科技股份有限公司 Linear flat-top light spot generation system, method and equipment based on Dammann grating
CN115113409B (en) * 2022-08-26 2022-12-30 成都莱普科技股份有限公司 Linear flat-top light spot generation system, method and equipment based on Dammann grating
CN116931286A (en) * 2023-09-15 2023-10-24 成都莱普科技股份有限公司 Beam shaping module, method and device
CN116931286B (en) * 2023-09-15 2023-11-24 成都莱普科技股份有限公司 Beam shaping module, method and device

Also Published As

Publication number Publication date
WO2019024359A1 (en) 2019-02-07

Similar Documents

Publication Publication Date Title
CN107290861A (en) Laser beam homogenization device and method
CN1330453C (en) Beam formation unit comprising two axicon lenses, and device comprising one such beam formation unit for introducing radiation energy into a workpiece consisting of a weakly-absorbent material
US7782535B2 (en) Device for beam shaping
DE112015000994T5 (en) Systems and methods for multi-beam laser arrays with variable beam parameter product
CN104181691B (en) Based on the folding scanning optics of MEMS micro mirror
US20100309559A1 (en) Device for Beam Shaping
CN102053371A (en) Titanium precious stone tunable laser light beam collimating and shaping system
CN107121781A (en) Light-beam forming unit
CN105892066A (en) Straight line laser generation device
DE102016102591A1 (en) Device for shaping laser radiation
CN104836114A (en) Fast-slow axis beam quality homogenizing device of semiconductor laser
CN207181837U (en) Laser beam homogenization device
US6324190B1 (en) Device with at least one beam source and an arrangement for geometric reshaping of the radiation field emitted by the beam source
CN110941097A (en) Conical view field emission optical system for laser panoramic detection
CN106291949B (en) A kind of apparatus for shaping of laser beam
CN104094161A (en) Method for designing laser-light-shaping optical component, method for producing laser-light-shaping optical component, and laser-light-shaping optical system
CN104953465A (en) Diode laser matrix beam uniformizing device based on spatial frequency spectrum segmentation process
CN113970871A (en) Light source system and projection system
US20200033585A1 (en) Optical article and illumination system for endoscope
US11249317B2 (en) Device for collimating a light beam, high-power laser, and focusing optical unit and method for collimating a light beam
CN103972780B (en) A kind of method being quickly found out laser pulse temporal overlapping positions by adjustable diaphragm
CN109381292A (en) Laser beam output coupler and coupling output method
CN113325593B (en) Laser beam splitting system based on free-form surface lens
DE102014008355B4 (en) Optical system for homogenizing the intensity of laser radiation
CN106654840B (en) A kind of target light echo ability value regulation light source emission system

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
RJ01 Rejection of invention patent application after publication

Application publication date: 20171024

RJ01 Rejection of invention patent application after publication