CN1749806A - Full internal reflection-refraction laser beam converter - Google Patents

Abstract

The present invention relates to laser beam shaping and coupling converter, especially laser beam expander (or reducer) to increase (or decrease) the diameter of laser beam, and belongs to the field of laser beam shaping and coupling technology. It is one cone transparent to incident light and features that its point angle and the incident light direction determine its function, its circle size depends on the incident laser diameter or outgoing laser diameter and the length is then determined. The converter has simple structure, low cost and high magnification, and may be used widely in laser beam diameter changing application.

Description

Full internal reflection-refraction laser beam converter

Technical field

The present invention relates to a kind of transducer that the laser beam of laser emitting is carried out certain shaping, coupling, particularly lasing beam diameter is enlarged or compress and make its so-called beam expander of being used widely (perhaps contract bundle device), belong to shaping, the coupling technique field of laser beam.

Background technology

As everyone knows, the angle of divergence and the bore that have a certain size from the laser beam of laser emitting often, if do not take certain shaping, coupling measure to be difficult to satisfy current many application to it, beam expander (perhaps contract bundle device) is then used it by lasing beam diameter being enlarged or compressing widely, so that the design and use of this quasi-converter seem is particularly important.As in some laser transmitting systems, need utilize beam expander expansion of laser light beam diameter, thereby the angle of divergence of compression light beam improves launch accuracy, survey laser weapon, environment measuring etc. as laser radar.Need to utilize the diameter that the bundle device compresses laser beam that contracts to make its laser beam that can be coupled into the very little optical fiber of diameter or obtain high energy intensity in other is used on the contrary, as fiber laser, laser plasma excites, laser surgery etc.

The employed laser beam expander of people roughly is divided into refractive and reflection-type two classes at present.The beam expander of refractive generally is to be formed by two or more combination of lensess, there are Galileo type and Kepler's type in typical refractive system, the advantage of refractive beam expander is that design, processing and the adjusting of instrument is all fairly simple, but multiplying power that this type systematic shortcoming is the expansion bundle is little, volume is big, because thereby the flaw of the anti-reflective film of lens incidence surface makes the part outgoing laser beam turn back to the damage that laser instrument causes laser instrument again, reduced the serviceable life of laser instrument in addition.The reflection-type beam expander is by secondary mirror and two reflector group of primary mirror and forms, compare refractive reflection-type beam expander and not only have higher expansion bundle multiplying power and big outgoing aperture, and volume is little, in light weight.But it is more widely used for spherical aberration corrector, coma and the official post of astigmatism iseikonia preferably, and this type of beam expander is generally all made aspheric system, as reflection-type aspheric surface Cassegrain system and Pascal Greggory system.But this type systematic causes the center shading easily, institute is so that occurred from axle Cassegrain system and Pascal Greggory system, though it is minimum from axle system energy loss to be dropped to, but limited and expanded bundle multiplying power and outgoing aperture, in addition because so the very little processing of size of secondary mirror is got up quite difficult, cost an arm and a leg, so this type of beam expander is not widely used.

Summary of the invention

The objective of the invention is to disclose a kind of new full internal reflection-refraction laser beam converter, overcome expansion bundle multiplying power that prior art exists low little, transfer efficiency is low, the processing difficulty of getting up costs an arm and a leg ... etc. defective.

Technical scheme of the present invention:

Full internal reflection-refraction laser beam converter, it be one to the transparent cone of incident light, L is the length of transducer, it is 2 α that cone is bored sharp angle, 2H is the diameter of cone disk, centre rotational axis is x, and its characteristics are levied and are: the size of boring sharp angle 2 α has determined the effect that it is concrete, n _εRefractive index for transducer; Relation between them depends on following formula

$n_{\mathrm{\ϵ}}\sin [\frac{\mathrm{\π}}{2}-(2n-1)\mathrm{\α}]=\sin (\frac{\mathrm{\π}}{2}-\mathrm{\α})(n=\mathrm{2,3},4,\·\·\·)$

Here n is the intersection point number of times of propagating light and sidewall, and different intersection point number of times multiplying powers is also different, and n is big more, and multiplying power is high more, and corresponding α is more little;

Regulate the size of α and the incident direction of change incident light, it is the key which kind of effect the decision transducer specifically plays, when incident light from disk along centre rotational axis incident from boring the side outgoing of point, and the angle α of awl point satisfy above-mentioned formula then transducer effect that directional light is played be the bundle that contracts; When incident light from the side of boring point along centre rotational axis incident from the disk outgoing, and the angle α of awl point satisfies following formula equally, then transducer effect that directional light is played is to expand bundle; When incident light from disk along centre rotational axis incident from bore the point the side outgoing, when the angle α of awl point no longer satisfies following formula, then the effect played of transducer is to converge directional light or make directional light convert hollow laser beam to, laser beam converge or the degree of dispersing by the size decision of α;

The size of disk is by the diameter decision of the diameter or the incident beam of outgoing beam, and the length L of transducer could be determined in view of the above.

The diameter 2H of cone disk is satisfying formula tg α=H/L, and greater than the diameter of incident beam, transducer plays the Shu Zuoyong that contracts; When 2H when satisfying formula tg α=H/L, and greater than the diameter of incident beam with expand the product of bundle multiplying power, transducer plays and expands Shu Zuoyong.

The length L of transducer is to be obtained the size of L after α and H determine again by formula tg α=H/L, and α determines the also refractive index n of transducer of back _εBy selected material decision, material must be transparent to incident light, and promptly material can be ignored to absorption of incident light; For same incident light, different transducer material satisfies the formula in the claim 1 equally then corresponding to different transducer dimensions; Under the prerequisite of the formula in satisfying claim 1, the size of refractive index is for incident light: transducer is by incident light transparent glass or plastics are constituted.

Beneficial effect of the present invention:

1. because this transducer is the nonimaging optics components and parts, so for along the parallel beam of x axle incident and Yan Buhui causes any deviation of light.

2. the transmission principle owing to transducer mainly is total internal reflection, so energy loss is little, and the transfer efficiency height.

3. the size of α has determined to expand the size of bundle multiplying power M, so can obtain higher expansion bundle multiplying power M by the α that makes transducer is less.

4. because transducer only is made of an optical component, so simple in structure, low price can be widely adopted.

5. the key of transducer is the size of α, makes it be used for different purposes so can suitably regulate α, as Fig. 3-shown in Figure 6.

In a word, full internal reflection-refraction laser beam converter is that performance is comparatively perfect in the similar beam expander.

Description of drawings

Fig. 1: transducer contour structures synoptic diagram;

Fig. 2: the parameter of transducer and ray tracing synoptic diagram;

Fig. 3: the bundle that contracts of the parallel beam of incident calculates simulation drawing;

Fig. 4: simulation drawing is calculated in the focusing of the parallel beam of incident;

Fig. 5: the parallel beam of incident converts the calculating simulation drawing of hollow beam to;

Fig. 6: the expansion bundle of the parallel beam of incident calculates simulation drawing;

Fig. 7: n and corresponding α and expansion bundle multiplying power M graph of a relation;

Fig. 8: the bundle that contracts of the non-parallel beam of incident calculates simulation drawing

Fig. 9: the expansion bundle of the non-parallel beam of incident calculates simulation drawing

Among the figure:

1. transducer 2. incident lights 3. emergent light L. are the length alpha of transducer. the diameter n of the sidewall of transducer and the angle x. centre rotational axis 2H. cone disk between the central shaft _ε. the refractive index of transducer

Embodiment

Below in conjunction with accompanying drawing the specific embodiment of the present invention is described further:

The processing of full internal reflection-refraction laser beam converter is fairly simple, can be with melting two kinds of daraf(reciprocal of farad) and reverse mould methods, and material is used incident light transparent glass or plastics, the refractive index n of the material that we select for use _ε=1.5.

The contour structures synoptic diagram of transducer as shown in Figure 1, it plays when the tip is exit end for incident end disc is to expand Shu Zuoyong, otherwise is the Shu Zuoyong that contracts.No matter be that the expansion bundle or the propagation principle of the bundle transducer foundation that contracts all are full internal reflection-refraction principles.Because the reversibility of light is an example in this compression rule to light beam with transducer.Supposing to have a beam diameter is 2H ₁Collimated laser beam incide the disk of transducer along the centre rotational axis direction, by total internal reflection principle incident light is transferred to the afterbody of transducer earlier, every angle through total reflection propagating light and sidewall _nJust reduce 2 α, work as _nLess than critical angle _i=arcsin (1/n _ε) time propagating light just reflect from sidewall, can make emergent light still be parallel to centre rotational axis by selecting suitable α size, the diameter of outgoing beam is 2H ₂, multiplying power M=H ₁/ H ₂Wherein, α is the sidewall of transducer and the angle between the central shaft, n _εRefractive index for transducer.

Utilize the method for ray tracing to study the transmission rule of directional light earlier by transducer.Set up coordinate system as shown in Figure 2, the center of disk is a true origin, and L is the length of transducer, and 2H is the diameter of disk, H ₁And H ₂Be respectively the radius of incident beam and outgoing beam, α is the angle of sidewall and x axle, (x ₀, y ₀) be the origin coordinates of incident ray, (x _n, y _n) (n=1,2,3 ...) be the intersecting point coordinate of transmission ray and beam expander; _n(n=1,2,3 ...) be the incident angle of transmission ray with respect to sidewall, ₃' be ₃The refraction angle; _n(n=1,2 ...) be the angle between transmission ray and the x axle, when light rotates in the counterclockwise direction to the x axle, just get, otherwise get negative.

Transmission ray is only followed two transmission rules in transducer inside:

1. work as y ₀Had in＞0 o'clock

$\left\{\begin{array}{c}{x}_{n+1}=\frac{H-{(-1)}^n(y_n-x_n\mathrm{tg}{\mathrm{\&theta;}}_n)}{\mathrm{tg\&alpha;}+{(-1)}^n\mathrm{tg}{\mathrm{\&theta;}}_n}\\ y_{n+1}=y_n+(x_{n+1}-x_n)\mathrm{tg}{\mathrm{\&theta;}}_n\\ \mathrm{\&theta;}={(-1)}^{\mathrm{<figure-callout\; id="2"\; label="n"\; filenames="A20051001552100082.png,A20051001552100083.png"\; state="\{\{state\}\}">n</figure-callout>}}2\mathrm{n\&alpha;}\end{array}\right.(n=\mathrm{0,1},2,\&CenterDot;\&CenterDot;\&CenterDot;)----\left(1\right)$

2.y ₀Had in＜0 o'clock

$\left\{\begin{array}{c}{x}_{n+1}=\frac{H+{(-1)}^n(y_n-x_n\mathrm{tg}{\mathrm{\&theta;}}_n)}{\mathrm{tg\&alpha;}-{(-1)}^n\mathrm{tg}{\mathrm{\&theta;}}_n}\\ y_{n+1}=y_n+(x_{n+1}-x_n)\mathrm{tg}{\mathrm{\&theta;}}_n\\ {\mathrm{\&theta;}}_n={(-1)}^{n+1}2\mathrm{n\&alpha;}\end{array}\right.(n=\mathrm{0,1,2},\&CenterDot;\&CenterDot;\&CenterDot;)----\left(2\right)$

Tg α=H/L wherein

This shows, need only the origin coordinates of given incident ray and the size of transducer, can go out the transmission situation of transmission ray by above-mentioned transmission rule recursion.As the incident angle of transmission ray with respect to sidewall _nTransmission ray just can come from the sidewall refraction during less than critical angle, and this moment, the coordinate of transmission ray and sidewall intersection point was (x _n, y _n), as the among Fig. 2 ₃, have

n _εsin _n＝sin _n′ (3)

Attention: y _nPositive and negative intersection point number of times decision by propagating light, y when n is odd number _n＞0, on the contrary y _n＜0.

As shown in Figure 2:

_n＝π/2-(2n-1)α (n＝1，2，3…) (4)

Make the deviation minimum of incident ray then must make emergent ray still be parallel to the outgoing of x axle, have

_n′+α＝π/2 (5)

Simultaneous formula (3) (4) (5) gets relational expression:

$n_{\mathrm{\&epsiv;}}\sin [\frac{\mathrm{\&pi;}}{2}-(2n-1)\mathrm{\&alpha;}]=\sin (\frac{\mathrm{\&pi;}}{2}-\mathrm{\&alpha;})(n=\mathrm{2,3,4}\&CenterDot;\&CenterDot;\&CenterDot;)----\left(6\right)$

Can learn that separating of formula (6) has or not array, α is more little, n is big more, as long as the sidewall of transducer and the angle α of axis satisfy formula (6), then this transducer just can will still transfer out with directional light along the parallel of axis incident, dwindled its beam diameter simultaneously, n is the intersection point number of times of propagating light and sidewall here.As seen the exit direction of emergent ray mainly by the tg α=H/L parameter decision of transducer, after α determines, can be determined the plane of incidence diameter 2H of transducer in advance according to the diameter of incident beam, and then its length L also can be determined.

Fig. 3 is for working as n=4,2H ₁During=1mm, the compression situation map to incident beam of computer simulation transducer.As seen from Figure 3: 1. transducer does not change the intensity distributions of parallel beam; 2. transducer can still blaze abroad all directional lights of going into to shine with directional light.This moment transducer plane of incidence diameter 2H=2mm, length L=8.22mm, refractive index n _ε=1.5.

By formula (6) as seen,, can make outgoing laser beam converge to the x axle and a bit obtain high-intensity luminous energy in place, perhaps obtain hollow laser beam, respectively as shown in Figure 4 and Figure 5 when the size of suitable adjusting α.

Utilize the reversible principle of light, what it played when the tip is exit end for incident end disc is to expand Shu Zuoyong, as shown in Figure 6.

Fig. 7 works as n=2,3 ... pairing α size was restrainted multiplying power M (M=H with expanding in 10 o'clock ₁/ H ₂) graph of a relation, wherein the unit of α is a radian.This shows that α reduces to slow down along with the increasing progressively of n, and expand bundle multiple beginning linear increasing progressively eventually, when n=9, expand bundle multiplying power M greater than 16, so the expansion bundle multiplying power of taper beam expander is higher.

More than research is the propagation condition of parallel beam by transducer.When the laser beam incident of certain angle of divergence size is arranged, its propagation characteristic is similar to beam propagation properties with traditional imaging beam expander, promptly when the reduced of light beam then its angle of divergence increase, then its angle of divergence reduces when the diameter of incident beam increases, respectively as Fig. 8 and shown in Figure 9, wherein the angle of divergence of incoming laser beam is 1 °, and diameter is 1mm.Different is that Lagrange invariant (being the diameter of light beam and the product of its angle of divergence) is being not constant, Lagrange invariant slightly reduces when the diameter of compression light beam, n is big more, and the amplitude that reduces is big more, Lagrange invariant slightly increases when the diameter of expanded light beam, the amplitude of the big more increase of n is also big more, as shown in Table 1, only with n=4,8 is example.L wherein ₀Be the Lagrange invariant of incident beam, L _dFor light beam is compressed Lagrange invariant after the certain multiple, L _mBe the Lagrange invariant after the extended certain multiple of light beam.

This transducer can also substitute multifiber coupled laser diode emitting laser bundle, and has dwindled their beam diameter simultaneously, enables to be coupled in the less optical fiber of diameter.

Table one: the Lagrange invariant of transmitting beam

n L ₀ L _d L _m

4 1mm×1°＝1 0.19555mm×4.676°＝0.91439 7.6354mm×0.14954°＝1.1418

8 1mm×1°＝1 0.10786mm×6.60854°＝0.712797 20.336mm×0.063°＝1.28168

Claims (5)

1. full internal reflection-refraction laser beam converter, it be one to the transparent cone of incident light, L is the length of transducer, it is 2 α that cone is bored sharp angle, 2H is the diameter of cone disk, centre rotational axis is x, it is characterized in that: the size of boring sharp angle 2 α has determined the effect that it is concrete, n _εRefractive index for transducer; Relation between them depends on following formula

$n_{\mathrm{\&epsiv;}}\sin [\frac{\mathrm{\&pi;}}{2}-(2n-1)\mathrm{\&alpha;}]=\sin (\frac{\mathrm{\&pi;}}{2}-\mathrm{\&alpha;})(n=\mathrm{2,3,4}\&CenterDot;\&CenterDot;\&CenterDot;)$

Here n is the intersection point number of times of propagating light and sidewall, and different intersection point number of times multiplying powers is also different, and n is big more, and multiplying power is high more, and corresponding α is more little;

Regulate the size of α and the incident direction of change incident light, it is the key which kind of effect the decision transducer specifically plays, when incident light from disk along centre rotational axis incident from boring the side outgoing of point, and the angle α of awl point satisfy above-mentioned formula then transducer effect that directional light is played be the bundle that contracts; When incident light from the side of boring point along centre rotational axis incident from the disk outgoing, and the angle α of awl point satisfies following formula equally, then transducer effect that directional light is played is to expand bundle; When incident light from disk along centre rotational axis incident from bore the point the side outgoing, when the angle α of awl point no longer satisfies following formula, then the effect played of transducer is to converge directional light or make directional light convert hollow laser beam to, laser beam converge or the degree of dispersing by the size decision of α;

The size of disk is by the diameter decision of the diameter or the incident beam of outgoing beam, and the length L of transducer could be determined in view of the above.

2. according to the said total internal reflection-refraction laser beam converter of claim 1, it is characterized in that: the diameter 2H of cone disk is satisfying formula tg α=H/L, and greater than the diameter of incident beam, transducer plays the Shu Zuoyong that contracts; When 2H when satisfying formula tg α=H/L, and greater than the diameter of incident beam with expand the product of bundle multiplying power, transducer plays and expands Shu Zuoyong.

3. according to the said total internal reflection-refraction laser beam converter of claim 1, it is characterized in that: the length L of transducer is to be obtained the size of L after α and H determine again by formula tg α=H/L, α determines back and H when satisfying claim 2, L can with H by formula tg α=H/L change.

4. according to the said total internal reflection-refraction laser beam converter of claim 1, it is characterized in that: the refractive index n of transducer _εBy selected material decision, material must be transparent to incident light, and promptly material can be ignored to absorption of incident light; For same incident light, different transducer material satisfies the formula in the claim 1 equally then corresponding to different transducer dimensions; Under the prerequisite of the formula in satisfying claim 1, the size of refractive index is for the not influence of conversion characteristics of incident light.

5. according to the said total internal reflection-refraction laser beam converter of claim 1, it is characterized in that: transducer is by incident light transparent glass or plastics are constituted.

Images