DEVICE FOR SHAPING A LASER RADIATION

Abstract

Device for shaping a laser radiation, comprising a first homogenizer with a first array of lenses and a second homogenizer with a second array of lenses through which the laser radiation passes through one after the other, a lens device which superimposes the laser radiation passed through the second array of lenses in a working plane, and a first prism and a second prism arranged between the second homogenizer and the lens device, wherein the laser radiation passed through the second array of lenses successively passes through the first and the second prism passes before impinging on the lens means.

Claims

1. Device for shaping a laser radiation, in particular for shaping a linear intensity distribution of a laser radiation, comprising a first homogenizer with a first array of lenses, the device being set up such that a laser radiation to be shaped passes through the first array of lenses, a second homogenizer with a second array of lenses, wherein the device is set up such that the laser radiation that has passed through the first array of lenses passes through the second array of lenses passes through, a lens device, the device being set up such that the laser radiation that has passed through the second array of lenses passes through the lens device, so that, for at least the partial radiations of the laser radiation that have passed through some of the lenses of the second array are superimposed in a working plane, characterized in that the device has a first prism and a second prism arranged between the second homogenizer and the lens device, the device being arranged to allow the lens passed through the second array, Laser radiation successively passes through the first and the second prism before it impinges on the lens device.

2. Device according to claim 1, characterized in that the prisms are set up to reduce the cross section and/or the divergence of the laser radiation at least partially in a first direction (x) to reduce or increase, in particular whereby increasing the divergence increases the length of the linear intensity distribution and reducing the divergence a reduction in the length of the linear intensity distribution is achieved.

3. Device according to claim 2, characterized in that the prisms are adapted to the divergence of the laser radiation passing through them at least partially in the first direction (x) by one To change a factor of between 0.5 and 2.0, in particular thereby changing the length of the intensity distribution line-shaped strength by a factor of between 0.5 and 2.0.

4. Device according to claim 1, characterized in that the lenses of the first array and the second array are each arranged side by side, in particular wherein the direction (x) in which the lenses of the first array and of the second array are arranged next to one another, corresponds to the first direction (x).

5. Device according to claim 1, characterized in that the lenses of the first array and the second array are cylindrical lenses whose cylinder axes are aligned parallel to one another, in particular where the cylinder axes extend in a second direction (y) perpendicular to the first direction (x).

6. Device according to claim 1, characterized in that the first prism is arranged in the device in such a way that partial radiation of the laser radiation passed through lenses of the second array arranged next to one another are not yet overlapped with one another at least in the first direction (x) when entering the first prism.

7. Device according to claim 1, characterized in that at least one of the prisms, preferably both prisms, Movable, preferably pivotable about an axis.

8. Device according to claim 7, characterized in that by the movement, in particular the pivoting, of the at least one prism, the factor by which the cross section of the prisms is changed by the laser radiation passing through.

9. Device according to claim 7, characterized in that the axis about which at least one of the prisms, preferably both prisms are pivotable, extends in the second direction (y).

10. Device according to claim 1, characterized in that the two prisms are of the same design, in particular have the same size and/or the same shape.

11. Device according to claim 1, characterized in that the distance between the lenses of the first array to the lenses of the second array of the focal length for at least some lenses, preferably all Lenses, the second array corresponds.

12. Device according to claim 1, characterized in that the lens device is positioned in the device in a Fourier arrangement, so that a distribution of the laser radiation in angular space is converted by the lens device into an intensity distribution in spatial space.

13. Laser device for generating an intensity distribution of a laser radiation in a working plane, in particular for generating a linear intensity distribution of a laser radiation in a working plane, comprising at least one laser light source and one Device for shaping laser radiation, characterized in that the device for shaping laser radiation is a device according to claim 1.

14. Laser device according to claim 13, characterized in that the laser device comprises two laser light sources which are set up to generate laser radiation with properties that differ from one another, for example with divergences or beam profiles that differ from one another, wherein the laser device is set up so that the laser beams impinge on the device adjacent to one another and the lens device superimposes both laser beams in the working plane, in particular superimposes them in the linear intensity distribution.

15. Laser device according to claim 13, characterized in that the device for shaping a laser beam comprises four prisms, two of which are used for one of the different laser beams are provided.

16. Laser device according to claim 13, characterized in that the device for shaping a laser radiation comprises two prisms which are provided for both of the mutually different laser radiations.

Description

BRIEF DESCRIPTION OF FIGURES

[0014] FIG. 1 shows a schematic side view of a first embodiment with drawn-in beams of a laser radiation to be shaped;

[0015] FIG. 2a shows two diagrams which schematically illustrate the distribution of the laser radiation behind the second homogenizer in the spatial space and in the angular space;

[0016] FIG. 2b shows two diagrams which schematically illustrate the distribution of the laser radiation behind the second prism in spatial space and in angular space in a first position of the two prisms;

[0017] FIG. 2c shows two diagrams which schematically illustrate the distribution of the laser radiation behind the second prism in spatial space and in angular space in a second position of the two prisms;

[0018] FIG. 3a shows a schematic side view of the embodiment according to FIG. 1 in a first position of the two prisms;

[0019] FIG. 3b shows a diagram in which the intensity of the laser radiation in the working plane is plotted in arbitrary units against the spatial coordinates in the longitudinal direction of the line of the linear intensity distribution in mm, with the two prisms being in the first position shown in FIG. 3a; FIG. 4a shows a schematic side view of the embodiment according to FIG. 1 in a second position of the two prisms;

[0020] FIG. 4b shows a diagram in which the intensity of the laser radiation in the working plane is plotted in arbitrary units against the spatial coordinates in the longitudinal direction of the line of the linear intensity distribution in mm, with the two prisms being in the second position shown in FIG. 4a;

[0021] FIG. 5 shows a schematic side view of a second embodiment with drawn-in beams of a laser radiation to be shaped.

DETAILED DESCRIPTION

[0022] Identical and functionally identical parts are provided with the same reference symbols in the figures. A Cartesian coordinate system is drawn into some of the figures for better orientation.

[0023] The embodiment of the device for shaping laser radiation shown in FIG. 1 comprises, in a manner known per se, a first homogenizer 1 with a first array 2 of lenses 3 and a second homogenizer 4 with a second array 5 of lenses 6. The device is set up so that a laser radiation 7 to be shaped passes through the first array 2 of lenses 3 and the second array 5 of lenses 6 in succession.

[0024] The lenses 3, 6 are arranged side by side in a first direction x. The lenses 3, 6 are cylindrical lenses, the cylinder axes of which extend in a direction y perpendicular to the first direction x, the second direction y extending out of the plane of FIG. The lenses 3, 6 therefore act in the first direction x. The laser radiation 7 essentially moves in a third direction z, which is perpendicular to the first and the second direction x, y.

[0025] It is entirely possible to provide spherical lenses or differently designed lenses instead of cylindrical lenses, which act both in the first direction x and in the second direction y.

[0026] In the figures, the first array 2 is arranged on the exit surface of the first homogenizer 1 and the second array 5 is arranged on the entry surface of the second homogenizer 4. It is certainly possible to arrange both arrays 2, 5 on the entry surfaces or the exit surfaces or to arrange the first array 2 on the entry surface of the first homogenizer 1 and the second array 5 on the exit surface of the second homogenizer 4. Furthermore, it can also be provided that only a single transparent substrate is provided, on the entry surface of which the first array 2 is arranged and on the exit surface of which the second array 5 is arranged.

[0027] There is also the possibility that, for example, arrays of lenses that act in the second direction y are arranged on the entry surface of the first homogenizer 1 and/or the exit surface of the second homogenizer 4. For example, these can be cylinder lenses whose cylinder axes extend in the first direction x.

[0028] All lenses 6 of the second array 5 have the same focal length. The distance between the two arrays 2, 5 from one another is equal to the focal length of the lenses 6 of the second array 5.

[0029] The device shown in FIG. 1 also comprises, in a manner known per se, a lens device 8 which, in the exemplary embodiment shown, is in the form of a plano-convex lens 8 in a Fourier arrangement. The lens device 8 superimposes, in a manner known per se, the partial radiations of the laser radiation 7 emanating from the lenses 6 of the second array 5 in a working plane (not shown) in the first direction x. In this case, a distribution of the laser radiation in angular space is converted into a distribution in local space in the working plane.

[0030] It is entirely possible to provide other forms of the lens, such as a biconvex lens. Furthermore, a lens system can also be provided instead of a single lens.

[0031] The device shown in FIG. 1 also comprises two prisms 9, 10 between the second homogenizer 4 and the lens arrangement 8, through which the laser radiation 7 passes in succession. In the embodiment shown, the prisms 9, 10 have the same size and the same shape, with the cross section seen in FIG. 1 continuing into the plane of the drawing in FIG.

[0032] The first prism 9 on the left in FIG. 1 is arranged in such a way that when the laser radiation 7 impinges on the entry surface 11 of the first prism 9, the partial radiations of the laser radiation 7 that have passed through lenses 6 of the second array 5 arranged next to one another in the first direction x are not yet overlapped with each other.

[0033] By suitably aligning the prisms 9, 10, it is possible to change the cross section and/or the divergence of the partial radiations emanating from each of the lenses 6, in particular to change the same for each of the partial radiations. This applies to the changes

[00002]$D_{\mathrm{in}}.Math.{?}_{\mathrm{in}}=D_{\mathrm{out}}.Math.{?}_{\mathrm{out}},$

[0034] D.sub.in is the extent of the partial radiation entering the prisms 9, 10 in the first direction x in spatial space,

[0035] ?.sub.in is the extent of the partial radiation entering the prisms 9, 10 in the first direction x in angular space,

[0036] D.sub.out is the extent of the partial radiation exiting from the prisms 9, 10 in the first direction x in spatial space, and

[0037] ?.sub.out is the extent of the partial radiation exiting from the prisms 9, 10 in the first direction x in angular space.

[0038] FIG. 2a shows the cross-section 12a or the extent D.sub.in of the partial radiation entering the prisms 9, 10 in the first direction x in the spatial domain. 2a shows the divergence 13a or the expansion in the partial radiation entering the prisms 9, 10 in the first direction x the angular space .sub.in.

[0039] FIG. 2b and FIG. 2b illustrate the effect of two different positions of the prisms 9, 10 on the partial radiation emerging from the prisms.

[0040] FIG. 2b shows the cross section 12b or the extent D.sub.out of the partial radiation emerging from the prisms 9, 10 in the first direction x in the spatial domain. 2b shows the divergence 13b or the expansion out of the partial radiation emerging from the prisms 9, 10 in the first direction x in the angular space ?.sub.out. It turns out that the divergence 13b is smaller than the divergence 13a. The smaller divergence 13b or the smaller extent in the angular space is converted by the lens device 8 into a distribution in the spatial space in the working plane, so that a smaller extent of a field in the working plane in the first direction x, in particular a smaller length of the linear intensity distribution results.

[0041] FIG. 2c shows the cross section 12c or the extent D.sub.out of the partial radiation emerging from the prisms 9, 10 in the first direction x in the spatial domain. 2c shows the divergence 13c or the expansion out of the partial radiation emerging from the prisms 9, 10 in the first direction x in the angular space ?.sub.out. It turns out that the divergence 13c is greater than the divergence 13a. The greater divergence 13c or the greater extension in the angular space is converted by the lens device 8 into a distribution in the spatial space in the working plane, so that a greater extension of a field in the working plane in the first direction x, in particular a greater length of the linear intensity distribution results.

[0042] This is illustrated in FIGS. 3a to 4b using the specific exemplary embodiment of a device for forming a line-shaped intensity distribution 14 of a laser radiation in a working plane.

[0043] FIG. 3a shows a device in which the prisms 9, 10 are in a first position. In this first position, the length of the linear intensity distribution 14 is somewhat greater than 700 mm, as can be seen from FIG. 3b.

[0044] FIG. 4a shows the same device as in FIG. 3a. However, the prisms 9, 10 in FIG. 4a are in a second position, which differs from the first position. In this second position, the length of the linear intensity distribution 14 is approximately 500 mm, as can be seen from FIG. 4b.

[0045] The different positions of the prisms 9, 10 can be achieved by pivoting the individual prisms 9, 10 about an axis which extends in the second direction y. In the positions shown in FIGS. 3a and 4, for example, the first prism 9 in FIG. 4a is pivoted clockwise relative to the prism 9 in FIG. 3a about a corresponding axis extending in the second direction y. Furthermore, in the positions shown in FIGS. 3a and 4, the second prism 10 in FIG. 4a is pivoted counterclockwise relative to the prism 9 in FIG. 3a about a corresponding axis extending in the second direction y.

[0046] FIG. 5 shows an embodiment, which differs from that in FIG. 1 in that instead of two prisms 9, 10, four prisms 9a, 9b, 10a, 10b are provided. In this case, two first prisms 9a, 9b are arranged next to one another in the first direction x. Furthermore, two second prisms 10a, 10b are arranged side by side in the first direction x.

[0047] Two laser beams 7a, 7b impinge on the device, which differ from one another, for example, in terms of their divergence or their beam profile. The first laser radiation 7a strikes the upper region of the first homogenizer 1 in FIG. 5, whereas the second laser radiation 7b strikes the lower region of the first homogenizer 1.

[0048] The device is set up so that the laser radiation 7a that has passed through the upper first prism 9a in FIG. 5 then passes through the upper second prism 10a in FIG. 5 and that the laser radiation 7b that has passed through the lower first prism 9b in FIG. passes through the lower second prism 10b in FIG. Furthermore, the device is set up so that the two laser beams 7a, 7b passed through the second prisms 10a, 10b pass together through the lens device 8 and are superimposed by it in the working plane, in particular in the linear intensity distribution.

[0049] It has proven to be very advantageous that a single lens device 8 in a Fourier arrangement superimposes two possibly very different laser beams 7a, 7b in a working plane, in particular in a linear intensity distribution in the working plane, while at the same time the corresponding positions of the prisms 9a, 9b, 10a, 10b the length of the line can be specified.

[0050] Provision can be made for the homogenizers 1, 4 to have differently designed areas for the different laser beams 7a, 7b, which are next to one another or at a distance from one another in the first direction x.

[0051] It can also be provided that the device for forming two different laser beams 7a, 7b does not comprise four prisms but only two prisms, not shown, which are provided in this case for both mutually different laser beams 7a, 7b.

[0052] There is also the possibility that in the embodiments shown in FIGS. 1, 3a, 4a and 5 further lenses for focusing the laser radiation or the laser radiations in the working plane and/or for shaping the laser radiation or the laser radiations regarding the second direction y are provided. These may not be shown for reasons of clarity.