CN201401667Y - Semiconductor laser array light beam shaping and illuminating system - Google Patents

Abstract

The utility model discloses a semiconductor laser array light beam shaping and illuminating system. The semiconductor laser array light beam shaping and illuminating system comprises a semiconductor laser array, an optical system for transforming divergence angles of fast axis light beams, a device for deflecting angles of light beams on the fast axis direction and an optical system for transforming slow axis divergence angles and deflecting the light beams on the slow axis direction. The semiconductor laser array light beam shaping and illuminating system has the key points that the effect that Gaussian beams of a plurality of laser units are partially superposed and folded is formed in a far field through controlling the deflexion degree of light beam transmission axial cords of each laser unit respectively on the fast axis direction and the slow axis direction, and thereby illuminating light beams which accord with visual field demands are formed. The semiconductor laser array lightbeam shaping and illuminating system has the characteristics of high efficiency, simple structure, low cost and integratable practicability, and is particularly applied as an illuminating light source of an area array imaging laser radar and a laser active illuminating and detecting system.

Description

A kind of beam shaping illumination system of semiconductor laser array

Technical field

The utility model relates to a kind of beam shaping illumination system of semiconductor laser array.

Background technology

Semiconductor laser array is in order to obtain integrated high-power output, the semiconductor laser output module that utilizes semiconductor laser element to utilize the connection in series-parallel form to form, have characteristics such as power output height, photoelectric transformation efficiency height, the laser intensity modulation is convenient, volume is little, the life-span is long, be suitable as very much the active lighting source of face battle array imaging laser radar and laser detection system.

The semiconductor laser laser instrument has special cavity resonator structure and working method, make the spatial distribution of light beam have asymmetry, (quick shaft direction) on the direction perpendicular to junction plane have 40 the degree about the angle of divergence, have the angle of divergence about 8 degree being parallel to (slow-axis direction) on the direction of junction plane, and light intensity is inhomogeneous in the angle of divergence separately.The far field light beam of the semiconductor laser stacked array after integrated also has similar spatial characteristics, and the far field light intensity presents the basic mode Gaussian distribution at quick shaft direction, and slow-axis direction generally presents the Hermitian Gaussian distribution.Reach good active illuminating effect, requirement light distribution in the illumination field of view angle is even, reach the high optical energy utilization efficiency that initiatively throws light on, and the illuminating bundle that needs restraint only appears in the illumination field of view angle.Therefore semiconductor laser array is applied to lighting use, comes original laser beam is carried out shaping with regard to adopting beam shaping illumination system.At present, along with being on the increase that semiconductor laser array is used in active detection system, the requirement of noise spectra of semiconductor lasers array beams shaping lighting engineering is also improving constantly.

Beam shaping lighting engineering at semiconductor laser array mainly contains two big class methods at present.In small field of view (below 3 degree * 3 degree) lighting use, the general collimating optical system that adopts, add microlens array at quick shaft direction and slow-axis direction, dispersion angle is all collimated compression to obtain the little angle of divergence, the shortcoming of this method is that the illumination field of view light intensity still presents Gaussian distribution, and is inhomogeneous.In big visual field illuminator, generally be earlier beam mode to be changed into even light to expand Shu Zhaoming again to the visual field of needs, as earlier with coupling light in the multimode fibre that semiconductor laser piles up, the mixed light effect of utilizing optical fiber repeatedly to reflect, obtain light intensity homogenising and pattern symmetrization at fiber-optic output, project to the field of illumination through optical system again.Because these class methods couple light to array in optical fiber or other light mixing cartridge, and this process technology difficulty height and coupling efficiency are low, the cost of manufacture height neither be very good as illuminator.

Summary of the invention

Conventional semiconductor laser array beam shaping illumination system efficient is not high in order to overcome, complex structure, not easy of integration, shortcoming that cost of manufacture is high, the purpose of this utility model is to provide a kind of beam shaping illumination system of semiconductor laser array, can improve the optical energy utilization efficiency of laser lighting significantly, and have simple in structure, cost of manufacture is low and can the integrated use of many pack modules to realize the characteristics of ultra-high power illumination.

The technical scheme that its technical problem that solves the utility model adopts is as follows:

One, a kind of beam shaping illumination system of semiconductor laser array:

Comprise the semiconductor laser two-dimensional array that equidistantly is arranged in parallel and in one plane forms by a plurality of semiconductor laser diode array justify aligns, microtrabeculae face lens arra, optical wedge array and cylindrical lens; Described semiconductor laser two-dimensional array, microtrabeculae face lens arra, optical wedge array, cylindrical lens are arranged in regular turn along the laser propagation direction, wherein each microtrabeculae face lens bus of microtrabeculae face lens arra and one by one alignment arrangement parallel with the line direction of semiconductor laser diode array, unit wedge in the optical wedge array and semiconductor laser diode array alignment are one by one arranged, and cylindrical lens bus and cylindrical lens optical axis vertical with semiconductor laser diode array overlaps with the perpendicular bisector of semiconductor laser diode array.

Described semiconductor laser diode array equidistantly is arranged on the one dimension line segment along slow-axis direction by a plurality of semiconductor laser elements and forms.

The numerical value of each wedge deviation angle in the described optical wedge array be one group from-0.5 θ _IFTo+0.5 θ _IFArithmetic progression, θ wherein _IFBe the illumination field of view angle of quick shaft direction, tolerance is θ _IFDeduct merchant after one divided by the semiconductor laser diode array number, deviation angle built-up sequence is any.

Two, another kind of beam shaping illumination system of semiconductor laser array:

Comprise that the semiconductor laser diode array justify align by the fast axle of a plurality of bands angle of divergence compression microtrabeculae face lens equidistantly is arranged in semiconductor laser two-dimensional array and the cylindrical lens of forming on the geometric surface shape pedestal; Described semiconductor laser two-dimensional array, cylindrical lens are arranged in regular turn along the laser propagation direction, and wherein vertical the and cylindrical lens optical axis of the semiconductor laser diode array of cylindrical lens bus and the fast axle of band angle of divergence compression microtrabeculae face lens overlaps with the perpendicular bisector that the fast angle of divergence of band is compressed the semiconductor laser diode array of microtrabeculae face lens.

The semiconductor laser diode array of the fast axle of described band angle of divergence compression microtrabeculae face lens, equidistantly be arranged on the one dimension line segment along slow-axis direction by a plurality of semiconductor laser elements and form, the optical axis of described microtrabeculae face lens is all the time on the laser propagation axis of the semiconductor laser diode array of correspondence.

Described geometric surface shape pedestal is one and fast axle angle of visual field θ _IFIn the protruding cylinder surface or the fluted column face of radian, the semiconductor laser diode array of the fast axle of described band angle of divergence compression microtrabeculae face lens equidistantly places on protruding cylinder surface or the fluted column face and keeps the laser propagation axis radially consistent with the face of cylinder; Described geometric surface shape pedestal or one and the fast axle of illumination field of view angle of visual field θ _IFDeng the protruding cylinder surface of radian or fluted column face cut after by branches such as semiconductor laser diode array total number with the fast axle angle of divergence compression microtrabeculae face lens cambered surface etc. polygonal right cylinder face, the semiconductor laser diode array of the fast axle of described band angle of divergence compression microtrabeculae face lens place respectively etc. polygonal right cylinder face each face the center and keep the laser propagation axis consistent with each face normal direction.

More than in two kinds of illuminators:

The effective focal length F of the line direction length dimension L of described semiconductor laser diode array, described cylindrical lens and slow-axis direction illumination field of view angle θ _ISRelation satisfy formula:

$\frac{L}{2F}=\tan \left(\frac{{\mathrm{\θ}}_{\mathrm{IS}}}{2}\right).$

The object distance Dx of described semiconductor laser diode array and described cylindrical lens satisfies relational expression:

$\mathrm{Dx}=\frac{L}{\mathrm{\α}\·\mathrm{Nx}\·{\mathrm{\θ}}_{\mathrm{os}}}-F$

Wherein α is a well-distributed coefficient of light, get the positive number less than 0.5, F is the effective focal length of described cylindrical lens, and Nx is the semiconductor laser unit number described in each described semiconductor laser diode array, L is the length dimension of described diode laser array, θ _OsBe the described semiconductor laser unit light beam slow axis angle of divergence before the shaping not.

The principles of science of the present utility model is:

The light beam model that can obtain semiconductor laser according to the boundary condition of fluctuation electromagnetic theory and semiconductor laser resonator is approximately Gaussian beam.The expression formula that Strength Space distributes is:

$I(x,y,z)=C_o\·{\left(\frac{w_0}{w\left(z\right)}\right)}^2\·\exp (-\frac{2r^2}{w^2\left(z\right)})---\left(1\right)$

Formula (1) is that the fundamental-mode gaussian beam propagated along the z axle is at point (x, y, z) intensity expression formula, wherein w ₀Be waist radius, $w^2\left(z\right)={\mathrm{<figure-callout\; id="0"\; label="w"\; filenames="Y2009201192070013H2.png,Y2009201192070014H2.png"\; state="\{\{state\}\}">w</figure-callout>}}_0^2[1+{\left(\frac{z}{z_0}\right)}^2],$ ${\mathrm{<figure-callout\; id="0"\; label="z"\; filenames="Y2009201192070013H2.png,Y2009201192070014H2.png"\; state="\{\{state\}\}">z</figure-callout>}}_0=\frac{\mathrm{\&pi;}{\mathrm{<figure-callout\; id="0"\; label="w"\; filenames="Y2009201192070013H2.png,Y2009201192070014H2.png"\; state="\{\{state\}\}">w</figure-callout>}}_0^2}{\mathrm{\&lambda;}}$ Be the Rayleigh distance C _oBe constant r ²=x ²+ y ²

Full-shape is dispersed in the far field ${\mathrm{\&theta;}}_{1/{\mathrm{<figure-callout\; id="2"\; label="e"\; filenames="Y2009201192070013H1.png,Y2009201192070014H1.png"\; state="\{\{state\}\}">e</figure-callout>}}^2}=2\frac{\mathrm{\&lambda;}}{{\mathrm{\&pi;\&omega;}}_0}.$ The angle of divergence of semiconductor laser quick shaft direction is: Being about 0.7 radian, λ=808nm Rayleigh distance is about 2um because z＞＞z ₀, then have $w\left(z\right)\&ap;{\left(\frac{w_0}{z_0}\right)}^2{\mathrm{<figure-callout\; id="2"\; label="z"\; filenames="Y2009201192070013H1.png,Y2009201192070014H1.png"\; state="\{\{state\}\}">z</figure-callout>}}^2,$ Substitution formula (1) can obtain the spatial distribution formula of Gaussian beam intensity under polar coordinates:

$I(\mathrm{\&rho;},\mathrm{\&theta;})=C_0{\left(\frac{z_0}{\mathrm{\&rho;}\cos \mathrm{\&theta;}}\right)}^2\exp (-2{\left(\frac{z_0}{w_0}\right)}^2{\mathrm{<figure-callout\; id="2"\; label="tan"\; filenames="Y2009201192070013H1.png,Y2009201192070014H1.png"\; state="\{\{state\}\}">tan</figure-callout>}}^2\mathrm{\&theta;})---\left(2\right)$

N=2K+1 semiconductor laser beam unit made K with fixed angle θ _dIncrease progressively deflection, K with fixed angle θ _dThe deflection of successively decreasing is the z axle in the direction of propagation of elementary beam, is that the light intensity stack result of any point of θ is perpendicular to point on the plane of z axle with respect to the deflection angle of z axle:

$I(z,\mathrm{\&theta;})=\underset{i=-\mathrm{<figure-callout\; id="0"\; label="K\; K\; C"\; filenames="Y2009201192070013H2.png,Y2009201192070014H2.png"\; state="\{\{state\}\}">K</figure-callout>}}{\overset{K}{\mathrm{\&Sigma;}}}{C}_{}^{}{}_0^{\&prime;}{\left(\frac{\cos \left({\mathrm{i\&theta;}}_d\right)}{z(1+\tan \mathrm{\&theta;}\tan \left({\mathrm{i\&theta;}}_d\right))}\right)}^2\exp (-\frac{8}{{\mathrm{\&theta;}}_{1/{\mathrm{<figure-callout\; id="2"\; label="e"\; filenames="Y2009201192070013H1.png,Y2009201192070014H1.png"\; state="\{\{state\}\}">e</figure-callout>}}^2}^2}\mathrm{ta}{n}^2(\mathrm{\&theta;}-{\mathrm{i\&theta;}}_d))---\left(3\right)$

Under z got certification condition, second was one to approximate is 1 approximate number in (3) expression formula, and its characteristic just depends mainly on $\underset{i=-K}{\overset{K}{\mathrm{\&Sigma;}}}\exp (-\frac{8}{{\mathrm{\&theta;}}_{1/{\mathrm{<figure-callout\; id="2"\; label="e"\; filenames="Y2009201192070013H1.png,Y2009201192070014H1.png"\; state="\{\{state\}\}">e</figure-callout>}}^2}^2}\mathrm{ta}{n}^2(\mathrm{\&theta;}-i{\mathrm{\&theta;}}_d)),$ This is the stack of Gaussian function more than,

Wherein α is even controlling elements, the appearance flat-top distribution waveform of expression formula when 0＜α＜0.5.So being a kind of many Gaussian beams, expression formula (3) is superimposed upon the way of realization that obtains even light distribution on the illuminated area.

Many Gaussian beams of light beam model called after angular deflection model of (3) statement, the characteristics of the light beam model of this specific character are at the dispersion angle that can pass through each Gaussian beam unit of control

And increase progressively deflection angle θ _dAnd the unit number is controlled the intensity uniformity in far field and the illumination field of view angle of total light beam.

The light beam model that utilizes the semiconductor laser element array to construct expression formula (3) respectively on fast axle and slow axis both direction is a cardinal principle of the present utility model, and quick shaft direction is more directly perceived, does not do explanation.Below slow-axis direction is made a concrete analysis of.

To described semiconductor laser diode array, light-emitting axis is Z, can be expressed as the stack of a following Nx Gaussian beam:

$I(x,z)={\mathrm{<figure-callout\; id="0"\; label="C"\; filenames="Y2009201192070013H2.png,Y2009201192070014H2.png"\; state="\{\{state\}\}">C</figure-callout>}}_0^{\&prime;}\&CenterDot;{\left(\frac{w_0}{w\left(z\right)}\right)}^2\&CenterDot;\underset{i=-\frac{\mathrm{Nx}-1}{2}}{\overset{\frac{\mathrm{Nx}-1}{2}}{\mathrm{\&Sigma;}}}\exp (-\frac{2{(x-i\&CenterDot;\frac{L}{\mathrm{Nx}})}^2}{w^2\left(z\right)})---\left(4\right)$

Satisfying under the paraxial condition, this light beam model can utilize abcd matrix optics to analyze in the propagation in space and the propagation by the geometric optics system, utilize lens transformation formula (4) that many Gaussian beams of flat-top model beams is converted to many Gaussian beams of angular deflection model beams

F□tan?Δθ _i＝i·d (5)

Wherein F is the lens effective focal length, $d=\frac{L}{\mathrm{Nx}}$ Be the spacing between each unit, Δ θ _iBe the deflection angle behind i unit light beam scioptics in the semiconductor laser diode array.With (5) formula, as id=L/2 and Δ θ _K=θ _IS/ 2, then obtain:

$\frac{L}{2F}=\tan \left(\frac{{\mathrm{\&theta;}}_{\mathrm{IS}}}{2}\right)---\left(6\right)$

Can determine the focal length F of lens with formula (6).

Formula (5) is updated to can obtains many Gaussian beams of flat-top model in the formula (4) through obtaining expression formula after the lens:

The light beam model of its statement of analysis result of expression formula (7) has (3) the represented light beam model profile characteristics that are similar to.The original beam of the laser cell ω that girdles the waist _O1Trend towards at 0 o'clock, can apply mechanically the geometric optical imaging formula, original slow axis angle of divergence θ _OsBe transformed to θ _s, can obtain the distance D x of semiconductor laser diode array and lens, original angle of divergence θ at last _Os, and the relational expression of even controlling elements α

$\mathrm{Dx}=\frac{L}{\mathrm{\&alpha;}\&CenterDot;\mathrm{Nx}\&CenterDot;{\mathrm{\&theta;}}_{\mathrm{os}}}-F---\left(8\right)$

Thereby realized the purpose of design of patent, obtained the even illumination in the angle of visual field limited range.

The utility model is compared the beneficial effect that has with background technology:

The utilization ratio height of 1 laser energy: because the optics number of process is few, and all be the transmissive optical components and parts of high percent of pass, efficient can reach about 80%, is far longer than 55% capacity usage ratio of prior art.

2 are convenient to realize modularization, integrated: make the same beam shaping illumination system of semiconductor laser array of many groups, the use that can directly walk abreast of each module, and the illumination uniformity in far field had the raising effect, be convenient to the far field illuminator of integrated super high power.

3 volumes are little, simple in structure, cost of manufacture is low: whole beam shaping lighting system structure is simple, and size is suitable with semiconductor laser array appearance and size.And the used device of the utility model all is the very ripe device of manufacture craft technology, and manufacturing cost is low, with respect to microlens array shaping illumination or semiconductor laser array fiber coupling module mode very big cost advantage is arranged all.

The utility model especially is suitable as the illuminating light source device of face battle array imaging laser radar system and remote active laser detection system.

Description of drawings

Below in conjunction with drawings and Examples the utility model is further specified.

Fig. 1 is the schematic perspective view that the utility model system constitutes.

Fig. 2 is the utility model quick shaft direction beam shaping principle schematic.

Fig. 3 is the utility model slow-axis direction beam shaping principle schematic.

Fig. 4 is the performance diagram of the utility model the principles of science expression formula (3).

Fig. 5 is a schematic diagram of realizing angular deflection device 5 in the utility model embodiment 2.

Fig. 6 is a schematic diagram of realizing angular deflection device 5 in the utility model embodiment 3.

Fig. 7 is the schematic diagram of the integrated use of multimode in the utility model embodiment 4.

Among the figure: 1, semiconductor laser two-dimensional array, 2, semiconductor laser element, 3, semiconductor laser diode array, 4, microtrabeculae face lens arra, 5, optical wedge array, 6, cylindrical lens, 7, the semiconductor laser diode array of the fast axle of band angle of divergence compression microtrabeculae face lens, 8, geometric surface type pedestal, 9, the integral illumination system unit.

The specific embodiment

Embodiment 1:

In Fig. 1, semiconductor laser two-dimensional array 1, microtrabeculae face lens arra 4, optical wedge array 5, cylindrical lens 6 are arranged in regular turn along the laser propagation direction, wherein each microtrabeculae face lens bus of microtrabeculae face lens arra 4 and one by one alignment arrangement parallel with the line direction of semiconductor laser diode array 3, unit wedge in the optical wedge array 5 and semiconductor laser diode array 3 alignment are one by one arranged, and vertical and cylindrical lens 6 optical axises of cylindrical lens 6 buses and semiconductor laser diode array 3 overlap with the perpendicular bisector of semiconductor laser diode array 3.The illuminator of setting up 10 degree * 10 degree with the 808nm semiconductor laser stacked array (stack) of 900W is an example, semiconductor laser two-dimensional array 1 is the 808nm semiconductor laser stacked array of 900W, the gross output of semiconductor laser diode array 3 is 100W, be to be made of the 1W semiconductor laser element 2 that 100 spacings are 100um, each semiconductor laser element 2 beam fast axis and slow axis dispersion angle are respectively θ _Of=40 degree and θ _Os=10 degree, 9 semiconductor laser diode array 3 are with equidistant composition 900W semiconductor laser two-dimensional array 1 altogether.Earlier will add microtrabeculae face lens arra 4 before the semiconductor laser diode array 3, compress its fast axle angle of divergence θ _fBe 3.5 degree, carry out beam deflection by optical wedge array 5 then, control module wedge angle makes that the angle of deflection is respectively i * 1.25 degree (i is respectively-4 ,-3 ,-2 ,-1,0,1,2,3,4), i.e. θ _Fd=1.25 degree.A cylindrical lens 6 is placed in the back, utilizes $\frac{L}{2F}=\tan \left(\frac{{\mathrm{\&theta;}}_{\mathrm{IS}}}{2}\right)$ Obtain focal length F=57.1mm, utilize again $\mathrm{Dx}=\frac{L}{\mathrm{\&alpha;}\&CenterDot;\mathrm{Nx}\&CenterDot;{\mathrm{\&theta;}}_{\mathrm{os}}}-F$ Dispersion angle θ after pressure is contracted _sBe 2 degree, then obtain the distance D x=42.8mm of cylindrical lens 6 and semiconductor laser two-dimensional array (1) light-emitting area, can obtain the even illuminating bundles of 10 degree * 10 degree.As shown in Figure 2 be beam shaping process at quick shaft direction, the laser beam that semiconductor laser diode array 3 sends earlier through microlens array 4 fast axle angle of divergence θ _fBoil down to 3.5 degree carries out deflection through optical wedge array 5 again, and to be equivalent to parallel flat inoperative for cylindrical lens 6 on this direction, and the reconstruct of overlapping of a plurality of Gaussian beams obtains even illuminating effect to final beam in the far field on quick shaft direction.As shown in Figure 3 be beam shaping process at slow-axis direction, i semiconductor laser element 2 on semiconductor laser diode array 3 from wheelbase from being d _i, according to d _iDifferent deflection angles takes place through the beam propagation axis behind the lens in difference, and the slow axis angle of divergence of each semiconductor laser element 2 is according to imaging $\mathrm{Dx}=\frac{L}{\mathrm{\&alpha;}\&CenterDot;\mathrm{Nx}\&CenterDot;{\mathrm{\&theta;}}_{\mathrm{os}}}-F$ Utilize Dx to adjust and carry out slow axis angle of divergence θ _OsCompressed transform, microtrabeculae face lens arra 4 and optical wedge array 5 are equivalent to optical parallel plate on this direction, for not contribution of beam shaping, the reconstruct of overlapping of a plurality of Gaussian beams obtains even illuminating effect to final beam in the far field on slow-axis direction.As shown in Figure 4 be that the reconstruct of overlapping of a plurality of Gaussian beams obtains the schematic diagram of even flat top beam.Can utilize in the practical operation and adjust uniformity and the border characteristic that Dx controls the far field illumination.

Embodiment 2:

In Fig. 1 semiconductor laser two-dimensional array 1, semiconductor laser element 2, semiconductor laser diode array 3, microtrabeculae face lens arra 5, the semiconductor laser diode array 7 and the geometric surface type pedestal 8 of the fast axle of the band shown in optical wedge array 6 usefulness Fig. 5, Fig. 6 angle of divergence compression microtrabeculae face lens replace.The illuminator of setting up 10 degree * 10 degree with the 808nm semiconductor laser stacked array (stack) of 800W is an example, wherein geometric surface shape pedestal 8 can be as shown in Figure 5 a protruding cylinder surface or a fluted column face with fast radian such as the axle angle of visual field 10 degree grade, the semiconductor laser diode array 7 of the fast axle of band angle of divergence compression microtrabeculae face lens equidistantly places on protruding cylinder surface or the fluted column face, also can be as shown in Figure 6 etc. the normal angle on wherein adjacent two planes of polygonal right cylinder face be θ _Fd=1.43 degree, the semiconductor laser diode array 7 of the fast axle of band angle of divergence compression microtrabeculae face lens place respectively etc. polygonal right cylinder face each face the center and keep the laser propagation axis consistent with each face normal direction, make the fast axle of band angle of divergence compression microtrabeculae face lens semiconductor laser diode array 7 the beam propagation axle on quick shaft direction, divide equally 10 and spend the angles of visual field.A cylindrical lens 6 is placed in the back, utilizes $\frac{L}{2F}=\tan \left(\frac{{\mathrm{\&theta;}}_{\mathrm{IS}}}{2}\right)$ Obtain focal length F=57.1mm, utilize again $\mathrm{Dx}=\frac{L}{\mathrm{\&alpha;}\&CenterDot;\mathrm{Nx}\&CenterDot;{\mathrm{\&theta;}}_{\mathrm{os}}}-F,$ Dispersion angle θ after pressure is contracted _s Be 2 degree, then obtain the distance D x=42.8mm of cylindrical lens 6 and semiconductor laser two-dimensional array 1 light-emitting area, can obtain the even illuminating bundles of 10 degree * 10 degree.Can utilize in the practical operation and adjust uniformity and the border characteristic that Dx controls the far field illumination.This embodiment has used one group of optical system less, has increased transmitance, and this platform machining is easy, and realizability is strong.

Embodiment 3:

As shown in Figure 7, be the integrated expansion of original system, a plurality of integral illumination system units 9 with same illumination field of view angle are formed the integrated use of array as the unit, with the general power that improves the far field illuminator and strengthen uniformity.

Claims (10)

1. beam shaping illumination system of semiconductor laser array, it is characterized in that: comprise the semiconductor laser two-dimensional array (1) that equidistantly is arranged in parallel and in one plane forms by a plurality of semiconductor laser diode array (3) justify align, microtrabeculae face lens arra (4), optical wedge array (5) and cylindrical lens (6); Described semiconductor laser two-dimensional array (1), microtrabeculae face lens arra (4), optical wedge array (5), cylindrical lens (6) is arranged in regular turn along the laser propagation direction, wherein each microtrabeculae face lens bus of microtrabeculae face lens arra (4) and one by one alignment arrangement parallel with the line direction of semiconductor laser diode array (3), unit wedge in the optical wedge array (5) and semiconductor laser diode array (3) alignment are one by one arranged, and cylindrical lens (6) bus and cylindrical lens (6) optical axis vertical with semiconductor laser diode array (3) overlaps with the perpendicular bisector of semiconductor laser diode array (3).

2. beam shaping illumination system of semiconductor laser array according to claim 1 is characterized in that: described semiconductor laser diode array (3) equidistantly is arranged on the one dimension line segment along slow-axis direction by a plurality of semiconductor laser elements (2) and forms.

3. beam shaping illumination system of semiconductor laser array according to claim 1 is characterized in that: the numerical value of each wedge deviation angle in the described optical wedge array (5) be one group from-0.5 θ _IFTo+0.5 θ _IFArithmetic progression, θ wherein _IFBe the illumination field of view angle of quick shaft direction, tolerance is θ _IFDeduct merchant after one divided by the semiconductor laser diode array number, deviation angle built-up sequence is any.

4. beam shaping illumination system of semiconductor laser array according to claim 1 is characterized in that: the line direction length dimension L of described semiconductor laser diode array (3), the effective focal length F and the slow-axis direction illumination field of view angle θ of described cylindrical lens (6) _ISRelation satisfy formula:

$\frac{L}{2F}=\tan \left(\frac{{\mathrm{\&theta;}}_{\mathrm{IS}}}{2}\right).$

5. beam shaping illumination system of semiconductor laser array according to claim 1 is characterized in that: described semiconductor laser diode array (3) satisfies relational expression with the object distance Dx of described cylindrical lens (6):

$\mathrm{Dx}=\frac{L}{\mathrm{\&alpha;}\&CenterDot;\mathrm{Nx}\&CenterDot;{\mathrm{\&theta;}}_{\mathrm{os}}}-F$

Wherein α is a well-distributed coefficient of light, get the positive number less than 0.5, F is the effective focal length of described cylindrical lens, and Nx is the semiconductor laser unit number described in each described semiconductor laser diode array, L is the length dimension of described diode laser array, θ _OsBe the described semiconductor laser unit light beam slow axis angle of divergence before the shaping not.

6. a beam shaping illumination system of semiconductor laser array is characterized in that: comprise that semiconductor laser diode array (7) justify align by the fast axle of a plurality of bands angle of divergence compression microtrabeculae face lens equidistantly is arranged in semiconductor laser two-dimensional array and the cylindrical lens of forming on the geometric surface shape pedestal (8) (6); Described semiconductor laser two-dimensional array, cylindrical lens (6) are arranged in regular turn along the laser propagation direction, and wherein vertical and cylindrical lens (6) optical axis of the semiconductor laser diode array (7) of cylindrical lens (6) bus and the fast axle of band angle of divergence compression microtrabeculae face lens overlaps with the perpendicular bisector that the fast angle of divergence of band is compressed the semiconductor laser diode array (7) of microtrabeculae face lens.

7. beam shaping illumination system of semiconductor laser array according to claim 6, it is characterized in that: the semiconductor laser diode array (7) of the fast axle of described band angle of divergence compression microtrabeculae face lens, equidistantly be arranged on the one dimension line segment along slow-axis direction by a plurality of semiconductor laser elements (2) and form, the optical axis of described microtrabeculae face lens is all the time on the laser propagation axis of the semiconductor laser diode array of correspondence.

8. beam shaping illumination system of semiconductor laser array according to claim 6 is characterized in that: described geometric surface shape pedestal (8) is one and fast axle angle of visual field θ _IFIn the protruding cylinder surface or the fluted column face of radian, the semiconductor laser diode array (7) of the fast axle of described band angle of divergence compression microtrabeculae face lens equidistantly places on protruding cylinder surface or the fluted column face and keeps the laser propagation axis radially consistent with the face of cylinder; Described geometric surface shape pedestal (8) or one and the fast axle of illumination field of view angle of visual field θ _IFDeng the protruding cylinder surface of radian or fluted column face cut after by branches such as semiconductor laser diode array (7) total number with the fast axle angle of divergence compression microtrabeculae face lens cambered surface etc. polygonal right cylinder face, the semiconductor laser diode array (7) of the fast axle of described band angle of divergence compression microtrabeculae face lens place respectively etc. polygonal right cylinder face each face the center and keep the laser propagation axis consistent with each face normal direction.

9. beam shaping illumination system of semiconductor laser array according to claim 6 is characterized in that: the line direction length dimension L of described semiconductor laser diode array, the effective focal length F and the slow-axis direction illumination field of view angle θ of described cylindrical lens (6) _ISRelation satisfy formula:

$\frac{L}{2F}=\tan \left(\frac{{\mathrm{\&theta;}}_{\mathrm{IS}}}{2}\right).$

10. beam shaping illumination system of semiconductor laser array according to claim 6 is characterized in that: the relational expression below the object distance Dx of described semiconductor laser diode array and described cylindrical lens (6) satisfies:

$\mathrm{Dx}=\frac{L}{\mathrm{\&alpha;}\&CenterDot;\mathrm{Nx}\&CenterDot;{\mathrm{\&theta;}}_{\mathrm{os}}}-F$

Wherein α is a well-distributed coefficient of light, get the positive number less than 0.5, F is the effective focal length of described cylindrical lens, and Nx is the semiconductor laser unit number described in each described semiconductor laser diode array, L is the length dimension of described diode laser array, θ _OsBe the described semiconductor laser unit light beam slow axis angle of divergence before the shaping not.

Images