LASER PACKAGE AND PROJECTOR WITH THE LASER PACKAGE

Abstract

A laser device comprises a plurality of laser diodes, each laser diode emitting a light beam having a fast axis and a slow axis and a beam direction; and one or more optical components configured to modify a divergence of the light beams in a fast axis plane and/or in a slow axis plane such that the light beams have a same focal plane in the fast axis plane and in the slow axis plane.

Claims

1. A laser device, comprising: a laser package comprising a plurality of laser diodes, each laser diode emitting a light beam having a fast axis and a slow axis and a beam direction; and one or more optical components configured to modify a divergence of the light beams in a fast axis plane and/or in a slow axis plane such that the light beams have a same focal plane in the fast axis plane and in the slow axis plane, wherein the laser diodes are mounted on one or more submounts, wherein the one or more submounts are arranged vertically on a base, wherein the one or more optical components comprise two cylindrical lenses or at least one cylindrical lens and a lens array, wherein at least one cylindrical lens of the one or more optical components is assigned to at least two laser diodes.

2. The laser device of claim 1, wherein at least one optical component is directly placed on the one or more submounts.

3. The laser device of claim 2, wherein the one or more submounts are arranged, along the vertical direction, between the base and the at least one optical component that is directly placed on the one or more submounts.

4. The laser device of claim 1, wherein at least one optical component forms a window of the laser package.

5. The laser device of claim 1, wherein the at least one cylindrical lens that is assigned to at least two laser diodes is a single cylindrical lens that is assigned to all laser diodes.

6. The laser device of claim 1, wherein the one or more optical components comprise a convergent optical component influencing only a beam divergence in the fast axis plane.

7. The laser device of claim 1, wherein the lens array comprises a plurality of convergent cylindrical microlenses arranged next to each other along a direction in the fast axis plane.

8. The laser device of claim 7, wherein each of the microlenses is assigned to at least one laser diode, wherein each of the microlenses has a cylinder axis that is perpendicular to the fast axis and parallel to the slow axis.

9. The laser device of claim 1, wherein, at an output surface of the lens array, the light beam of at least one laser diode is tilted in the fast axis plane with respect to the light beam of another of the laser diodes at the output surface of the lens array and/or with respect to an optical axis of the assigned microlens.

10. The laser device of claim 9, wherein at least some of the laser diodes are tilted with respect to each other in the fast axis plane.

11. The laser device of claim 9, wherein at least one laser diode is arranged off-centered in the fast axis plane with respect to the optical axis of the assigned microlens.

12. The laser device of claim 1, wherein the lens array comprises a plurality of microlenses that have different optical powers.

13. The laser device of claim 1, wherein at least some of the laser diodes are tilted with respect to each other in the slow axis plane.

14. The laser device of claim 1, wherein the one or more optical components comprise a divergent optical component influencing only a beam divergence in the slow axis plane.

15. The laser device of claim 1, wherein the one or more optical components comprise a divergent cylindrical lens assigned to all laser diodes.

16. The laser device of claim 1, wherein one or more of the plurality of laser diodes are tilted at an angle from an axis of symmetry of the one or more optical components.

17. The laser device of claim 1, further comprising a prism having two reflecting sides, onto which the laser diodes emit light, wherein on each side there are several faces that are tilted with respect to each other.

18. A projector comprising the laser device of claim 1, wherein for the light beams an aperture in the fast axis plane and an aperture in the slow axis plane overlap.

19. A laser device, comprising: a laser package comprising a plurality of laser diodes, each laser diode emitting a light beam having a fast axis and a slow axis and a beam direction; and one or more optical components configured to modify a divergence of the light beams in a fast axis plane and/or in a slow axis plane such that the light beams have a same focal plane in the fast axis plane and in the slow axis plane, wherein at least two laser diodes emit light beams that are arranged next to each other in a direction in a first plane, wherein the one or more optical components comprises a lens that is assigned to the at least two laser diodes and that has a curvature that lies is a second plane that is the same plane as the first plane.

20. The laser device of claim 19, wherein the lens is a cylindrical lens having a cylinder axis, wherein the cylinder axis is perpendicular to the first plane.

Description

BRIEF DESCRIPTION OF THE FIGURES

[0031] FIG. 1 illustrates a projector in accordance with various embodiments.

[0032] FIG. 2 illustrates an example of the placement of laser diodes side-by-side in a laser device in accordance with further embodiments.

[0033] FIG. 3 illustrates the beam divergence of a laser device in accordance with further embodiments.

[0034] FIG. 4 illustrates examples of modifying the fast and slow axes of a six-laser device in accordance with further embodiments.

[0035] FIG. 5 illustrates a system and method for modifying the field of view of both the fast and slow axes of a laser device in accordance with further embodiments.

[0036] FIGS. 6A and 6B illustrate further embodiments for the correction of differing divergences along the fast axis and the slow axis of a laser device using optics in accordance with various implementations.

[0037] FIG. 7 illustrates examples of implementing a laser beam tilt in a laser device in accordance with further embodiments.

[0038] FIG. 8 illustrates a further embodiment for the correction of differing divergences along the fast axis and the slow axis of a laser device using optics in accordance with various implementations.

[0039] FIG. 9 illustrates a further embodiment for the correction of differing divergences along the fast axis and the slow axis of a laser device using optics in accordance with various implementations.

[0040] FIG. 10 illustrates a further embodiment for modifying the field of view of both the fast and slow axes of a laser device in accordance with various implementations.

[0041] FIG. 11 illustrate laser devices according to further embodiments.

DETAILED DESCRIPTION

[0042] These and other features of the present implementations will be understood better by reading the following detailed description, taken together with the figures herein described. The accompanying drawings are not intended to be drawn to scale. For purposes of clarity, not every component may be labeled in every drawing.

[0043] In the following, various embodiments of a laser device and of a projector are described, wherein the laser device can be used in the projector as light source. The projector can be a display system in general and, in particular, a near-eye display system that is based on side-by-side scanning laser-beams. By way of example, even if not always explicitly shown, the laser device according to the depicted embodiments can comprise three laser diode sets, each having two laser diodes that are formed by edge-emitting diode lasers, respectively. Consequently, by way of example, six laser diodes can be used in a laser device according to the shown embodiments. However, other numbers of laser diode sets and laser diodes per laser diode set are also possible.

[0044] In the following, laser diodes are denoted with the reference numeral 10, to which, for example depending on the depicted view, further information can be added like, for instance, “a”, “b”, “R”, “G”, or “B”. In this regard, for instance a plurality of laser diodes can be denoted as “laser diodes 10a” or “laser diodes 10b” in one figure for indicating arrangement properties, while the same plurality of laser diodes, for instance the laser diode(s) 10a shown in the one figure, can be denoted as “laser diode 10R”, “laser diode 10G” and “laser diode 10B” in another figure for indicating color properties of those laser diodes.

[0045] FIG. 1 shows in a view 15 an exemplary embodiment of a projector in a projection application. Laser diodes (indicated by an emission plane EP) of a laser device emit a divergent beam through a window 12 of the laser device, wherein the beam is then reflected by reflector 14. Lenses 16 focus the reflected beam onto two orthogonal scanning mirrors 18a, 18b. Alternatively, here and in the following embodiments a single two-axis scanning mirror can also be used. In such case, a single reflecting small mirror replaces the two scanning mirrors 18a and 18b shown in FIG. 1. Moreover, reflector 14 can be omitted so that the laser diodes can emit the produced light directly onto the lenses 16. The focusing beam angle is modified by field-lens 20 before being focused onto micro-lens-array (MLA) 22. The MLA 22 therefore forms a focal plane. A more divergent beam emerging from the MLA 22 is collimated by optics 24 forming a relay-optics before exiting the projector and, for instance, entering a waveguide (not shown) that projects the image onto an observers' eye.

[0046] There is an optical path from the laser diodes, represented by emission plane EP, to the MLA 22. The limiting apertures in this optical path are the scanning mirrors, and, particularly, the resonant scanning mirror 18a that is the smallest optical component. Therefore, the superposition of all the beams from the laser diodes should have a minimum beam size at the position of at least one of the mirrors 18a, 18b, should illuminate the mirrors 18a, 18b with minimal “spillover” (causing power loss) and should focus on the MLA 22, i.e., the focal plane. The minimum beam size of the light beam emitted by the laser device, comprising the light beams of all operated laser diodes, can also be denoted as minimum aperture or, short, as aperture in the following. As mentioned above, all features and embodiments explained before and in the following are also applicable in case that the scanning mirrors 18a and 18b are replaced by a single two-axis scanning mirror.

[0047] FIG. 2 illustrates in a side view 25 and in a front view 27 an exemplary embodiment of a laser device comprising a laser package comprising three laser diode sets, wherein each of the laser diode sets comprises two laser diodes. By way of example, the laser package of the laser device further comprises a base 11, a prism 28 and a window 12. The layout shown in FIG. 2 is only an example and other architectures are possible for the placement and number of the laser diodes as well as for the components of the laser package.

[0048] The laser diodes are placed side-by-side in the laser package on the base 11. The laser diodes form two sets of three RGB lasers, on opposing reflecting sides of the prism 28 on the base 11. When operated, each of the laser diodes emits a light beam onto a reflecting side of the prism that reflects the light beams toward the window 12. In the side view 25 only two laser diodes 10a, 10b are visible, wherein the additions “a” and “b” denotes the side of the laser diodes with respect to the prism 28 on the base 11. The three laser diodes 10a on the left-hand side of the prism 28 emit red, green and blue light, respectively, and form one RGB configuration. The three laser diodes 10b on the right-hand side of the prism 28 form another RGB configuration. One of the RGB configurations can be seen in front view 27. In particular, the laser diodes of the shown RGB configuration are denoted as “10R”, “10G” and “10B”. Each pair of two laser diodes 10a, 10b emitting the same color forms a laser diode set, also denoted as color channel. Furthermore, each of the depicted laser diodes 10a, 10b represents an RGB set comprising a red-emitting laser diode, a green-emitting laser diode and a blue-emitting laser diode. Consequently, in the following it will also be referred to “laser diode group 10a” and “laser diode group 10b”.

[0049] As can be seen in the front view 27, each of the laser diodes 10R, 10G, 10B is placed on a submount 26. The submounts 26 may preferably be placed vertically on the base 11 in the laser package. As explained above, this means that the base 11 has a base surface, on which the submounts are arranged and which defines a horizontal plane of the laser package and, thus, of the laser device. The laser diodes are arranged on mounting surfaces of the submounts, wherein the mounting surfaces of the submounts are not parallel to the base surface. Preferably, the mounting surfaces are perpendicular to the base surface. The light emitted from the laser diodes is reflected perpendicularly by prism 28 and passes through the window 12 already indicated in FIG. 1. In other words, the light emitted from the laser diodes and, thus, from the laser package is emitted from the window 12 onto the further optical components described in connection with FIG. 1.

[0050] The arrangement of the six laser diodes (three on each side of prism 28) generates a six spot pattern 32 where every spot must be as sharp as possible to enable a sharp scanned image. Every spot is marked with the reference numeral 200 followed by additions according to the respective color (R, G or B) and the respective RGB set (a or b). Pattern 36 shows a different pattern that can be generated when two laser diodes are placed on every submount 26. A single RGB set is also possible in which there are only three or four laser diodes (not shown in FIG. 2). In the following, for the sake of clarity, the description of the laser device and the projector will focus on the six-laser configuration as shown in views 25 and 27 and in pattern 32.

[0051] FIG. 3 illustrates the beam divergence of a laser device and a modification of the beam divergence in accordance with various implementations. Diagram 39 shows a diode laser 10 that typically transmits a non-symmetric beam diverging fast on one axis F, the so-called fast axis, and diverging slow on another axis S, the so-called slow axis. This asymmetric beam divergence causes substantial power loss since not all the light can be collected by the projector's optics.

[0052] Diagram 41 shows a method utilizing two cylindrical lenses 44 and 46 for converting the elliptical beam into a circular beam. Diagram 48 shows the same configuration but with different conventions: the solid lines represent the fast axis rays, i.e., the beam in the fast axis plane, while the dashed lines represent observation from the side where the slow axis is visible, i.e., the beam in the slow axis plane. The lenses 44, 46 are depicted as double headed arrows, only in that view in which they are optically effective. Thus, lens 44, which effects the emitted light only with regard to the fast axis, is only shown in the fast axis plane view, whereas lens 46, which effects the emitted light only with regard to the slow axis, is only shown in the slow axis plane view. In the following figures the same convention of depicting cylindrical lenses is used.

[0053] Diagram 50 show an alternative configuration where both cylindrical lenses are active on the fast axis plane, but wherein one is a convergent lens 52 and the other one is a divergent lens 54. This modifies the fast axis to overlap the slow axis (which is unchanged) in terms of angle and point of origin.

[0054] Heron, for clarity, most configurations depicted are equivalent to the configuration according to diagram 50 where only the fast axis is manipulated. However, similar optical arrangements may include the manipulation of both axes as depicted in diagrams 41 and 48, wherein the axis of the second lens is parallel to the slow axis.

[0055] FIG. 4 illustrates exemplary embodiments for modifying the fast and slow axes of a laser device, i.e., for modifying the light beams emitted by the laser diodes in the fast axis plane and in the slow axis plane, wherein the laser device comprises six laser diodes. Diagram 52 illustrates schematically how the array of six laser diodes shown in FIG. 2, which have their fast axis planes overlapping, can be modified based on configuration 50 in order to have circular beams. It is apparent that the distance between the R, G and B laser diodes should be large enough so that their beams do not overlap when being refracted by second lenses 54. However, the two laser diode groups 10a and 10b can be very close. Consequently, prism 28 can be narrow.

[0056] Diagram 56 shows the same six-laser device having both the fast and slow axes modified as implemented in the configurations shown in diagrams 41 and 48 of FIG. 3. Using a single cylindrical lens for the fast axis allows the distance between the R, G and B laser diodes to be closer. However, the presence of lens 46 along the slow axis means that the laser diode groups 10a and 10b must be spaced further apart. The laser diodes' beams have approximately a Gaussian angular distribution. Thus, implementing lenses adjacent to each other will cause leakage of one beam to the lens of a neighboring laser diode, thereby causing crosstalk and degradation of the projected image. Consequently, the laser diodes have to be placed further apart when attempting the depicted beam modification.

[0057] FIG. 5 illustrates a system and method for modifying the field of view of both the fast and slow axes of a laser device in accordance with various implementations. Diagram 58 in FIG. 5 shows a set of parallel divergent beams 60 being refracted by an array of lenses 62 to generate a set of parallel less-divergent beams 64. Diagram 65 shows an arrangement that produces the same optical result as the arrangement of diagram 58, except that the set of divergent beams 66 enter a single lens 68, the lens 68 having its optical power on the same plane as the distribution of beams 66 emitted by at least two laser diodes and, preferably, of more than two or even all laser diodes of the laser device. In other words, the lens 68 is assigned to at least two laser diodes and, preferably, to more than two or even all laser diodes of the laser device. That the lens 68 has its optical power on the same plane as the distribution of two or more beams means that the two or more light beams are arranged next to each other in a direction in a first plane and the curvature of the lens lies in a second plane that is the same plane as the distribution of beams, as can be easily seen in diagram 65. In case of a cylindrical lens 68 having a cylinder axis, the first plane, i.e., the plane in which the direction lies along which the beams are arranged next to each other, is perpendicular to the cylinder axis of the cylindrical lens 68.

[0058] In order to have the same set of parallel less-divergent beams 64 exit from the single lens 68 as from the array of lenses 62 shown in diagram 58, the beams 66 enter the single lens 68 at tilted angles. Although in FIG. 5 converging lenses 62, 68 are shown, a corresponding effect can be obtained in case of diverging lenses.

[0059] FIG. 6A illustrates an embodiment for the correction of differing divergences along the fast axis and the slow axis of a laser device in a projector using optics in accordance with various implementations. Diagram 70 shows the fast axis orientation with correction. The RBG laser diodes 10 of the laser device emit light onto a convergent optical component, which reduces the fast axis divergence. In the shown embodiment, the convergent optical component is formed by a lens array 72. The lens array 72 comprises convergent cylindrical microlenses arranged next to each other in the plane of the fast axis, wherein the effect of the microlenses is equivalent to the function of the lenses 52 in FIG. 3. Consequently, the cylindrical microlenses each have a cylinder axis that is perpendicular to the fast axis and parallel to the slow axis of the light emitted by the laser diodes. Each of the microlenses is assigned to a laser diode. In contrast to individual lenses, the lens array 72 can be more compact, thereby allowing a more compact design of the laser device.

[0060] Preferably, the lens array 72 comprising the microlenses is a part of the laser device and can be arranged, for instance, below or on the window 12. Alternatively, the lens array 72 can form the window 12. It can also be possible that the lens array 72 is a part of the projector and is arranged downstream of the laser device with respect to the beam direction of the light emitted by the laser device.

[0061] Downstream of the convergent optical component, i.e., the lens array 72 in the shown embodiment, a further optical component is arranged that is assigned to all laser diodes. The further optical component is formed by a single divergent cylindrical lens 74 in the shown embodiment. The light beams exiting the lens array 72 enter the single divergent cylindrical lens 74, which has a cylinder axis that is also perpendicular to the fast axis and parallel to the slow axis of the light emitted by the laser diodes. The single divergent cylindrical lens 74 replaces the set of divergent lenses 54 in FIG. 3. In contrast to individual lenses, the single lens 74 can be more compact, thereby allowing a more compact design of the laser device.

[0062] Preferably, the lens 74 can also be a part of the laser device and can be arranged, for instance, below or on the window 12. The lens array 72 and the single lens 74 can be placed on the same side of the window 12 with respect to the beam direction of the light emitted by the laser device, or on different sides of the window. Alternatively, the lens array 72 can form the window 12. It can also be possible that the lens 74 is a part of the projector and is arranged downstream of the laser device with respect to the beam direction of the light emitted by the laser device. Lens 74 can also be a converging lens orientated along the slow axis (equivalent to diagrams 41 and 48).

[0063] Lens 16 of the projector focuses the laser beams emitted from the single lens 74 onto the MLA plane 22. The minimum aperture of the set of beams in the fast axis plane is indicated by reference numeral 76. Preferably, the scanning mirror 18a may be located at this location when the fast axis orientation is taken into account. However, diagram 78 shows that in the slow axis orientation, which has the same focus plane formed by the MLA plane 22 as diagram 70, the location of the minimum aperture 80 of the set of beams in the slow axis plane is not at the same position as the aperture 76 for the fast axis orientation. Thus, the scanning mirror 18a may preferably be located at this other location when the slow axis orientation is taken into account. Consequently, since the apertures of the six lasers in the slow axis orientation and in the fast axis orientation do not overlap, both possibilities, i.e., placing a scanning mirror either at the position of the aperture 76 with respect to the fast axis of the emitted light or at the position of the aperture 80 with respect to the slow axis of the emitted light, are not perfect with respect to the respective other orientation, so that energy will spill over at the scanning mirror.

[0064] Diagram 82 shows an implementation of the principles described with respect to FIG. 5. The beams of at least one or more of the laser diodes are tilted in the fast axis plane at the output surface of the convergent optical component formed by the lens array 72. This means that the light beams emitted by at least one of the laser diodes exits the convergent optical component in a direction that is not parallel to the optical axis of the convergent optical element. In case of the shown lens array 72 the light beam emitted by at least one of the laser diodes exists the assigned microlens in a direction that is not parallel to the optical axis of that microlens. In particular, the light beams of at least one or more of the laser diodes can also be tilted in the fast axis plane at the input surface of the convergent optical element formed by the lens array 72. In the shown embodiment, the tilting of at least one or more of the light beams is effected by tilting some of the laser diodes (labeled 10RT, 10GT) with respect to each other in the plane of the fast axis as indicated in diagram 82.

[0065] A light beam of a laser diode being tilted at the input or output surface of the convergent optical component can mean that the beam direction of the tilted beam deviates from the beam direction of a light beam emitted by another laser diode at the input or output surface of the convergent optical element. In particular, in case of a lens array as shown in FIG. 6A, a light beam of a laser diode being tilted can mean that the beam direction of the tilted light beam deviates, at the input or output surface of the lens array, from the optical axis of the assigned microlens of the lens array. A laser diode being tilted can mean that the main emission direction of the light emitted by the tilted laser diode is not parallel to the main emission direction of the light emitted by another laser diode. The main emission direction of a laser diode is the beam direction of the light beam when exiting the laser diode.

[0066] As consequence of tilting some of the light beams, for instance by tilting some of the laser diodes, the focal plane given by the MLA plane 22 is maintained at the same location, but the minimum aperture 84 of the set of beams in the fast axis plane can be shifted, for instance closer to the laser diodes. By adjusting the tilting angle of the tilted laser diodes, the shift of the aperture 84 can be optimized so that it overlaps with the slow axis aperture 80 in diagram 78. Now, the superposition of all laser diode beams has an overlapping minimum aperture in the fast axis plane and in the slow axis plane and minimum light power is lost, when a scanning mirror is placed at the position of the overlapping aperture.

[0067] FIG. 6B illustrates a further embodiment for the correction of differing divergences along the fast axis and the slow axis of a laser device using optics in accordance with various implementations. As shown in diagram 83, the light beam emitted by laser diode 10 enters the microlens of lens array 72B, forming the convergent optical component, off-centered in the fast axis plane with respect to the optical axis (indicated by the dashed line) of the microlens. In the shown embodiment, this is effected by arranging the laser diode 10 off-centered in the fast axis plane with respect to the optical axis of the microlens lens, thereby generating a beam tilt at the output surface of the lens array 72 and thus behind the lens array 72B. This principle is implemented in the laser device of the projector shown in diagram 84, where all the lasers (10RS, 10G and 10BS) are arranged parallel with a predefined spacing, while the microlenses of the lens array 72B have a spacing that is slightly smaller. Consequently, the beams from lasers 10BS and 10RS are arranged off-centered and, thus, are tilted to be convergent (equivalent to the effect of tilting the laser diodes 10RT and 10BT in diagram 82), while the light beam from laser diode 10G is not off-centered and, thus, continues without tilt. The same approach can be used for different shifts from the center for the laser diodes 10R and 10B depending on the chromatic dispersion or other aberration effects. Also, the spacing of the microlenses can be wider, if diverging beams are needed. The chromatic aberration can be compensated if the microlenses of lens array 72/72B have different optical powers.

[0068] FIG. 7 illustrates exemplary embodiments of implementing the described light beam tilt in a laser device in accordance with various implementations. Diagram 86 shows a placement of the lasers and submounts 26 at differing relative angles with respect to the central parallel prism 28A. For the sake of clarity, only laser diode 10aRT, corresponding to laser diode 10RT shown in FIG. 6A, is labelled.

[0069] Diagram 88 shows a parallel placement of the laser diodes while the prism 28B has modified faces reflecting the light from every laser diode at the desired respective correct (tilted or non-tilted) angle. Diagram 90 is a close-up view of prism 28B. As can be seen, the prism 28B has two reflecting sides, onto which the laser diodes emit light, wherein on each side there are several faces 94 that are tilted with respect to each other. The faces 94 of prism 28B are additionally marked according to the assigned laser diodes by color (R, G and B) and side (a and b).

[0070] Diagram 96 shows an example with exemplary dimensions for lens array 72 that may be placed adjacent to window 12 or embedded in it. In this preferred configuration of the array, every cylindrical array acts simultaneously on two opposing laser diodes from both sides of the prism.

[0071] FIG. 8 illustrates a further embodiment for the correction of differing divergences along the fast axis and the slow axis of a laser device using optics in accordance with various implementations. FIG. 8 includes a reproduction of diagram 70 of FIG. 6A and a new diagram 100 that shows two laser diode groups 10aT, 10bT that are tilted with respect to each other in the slow axis plane. The two laser groups 10aT, 10bT are tilted so that the aperture 102 in the slow axis plane, i.e., the apertures of laser diode groups 10a and 10b, overlap with the aperture 76 in the fast axis plane (R, G, B in every group) of FIG. 6. Therefore, all six lasers' apertures are overlapping.

[0072] FIG. 9 illustrates a further embodiment for the correction of differing divergences along the fast axis and the slow axis of a laser device using optics in accordance with various implementations. In diagram 104, the laser diodes (only the visible laser diodes 10aRW and 10bBW are labeled) are tilted on the submount 26 with respect to a horizontal plane defined by a base, for instance base 11 shown in FIG. 2, on which the submounts 26 are mounted. In this way the light beams hit the prism 28 (a or b) at specified angles and are reflected at specified angles. Alternatively, as shown in diagram 106, also a configuration is possible where the prism's 28 reflecting surfaces include at the top of the prism 28 an angle that deviates from 90°, so that the reflected beams receive the desired angles, whereas the laser diodes can be mounted horizontally, i.e., to emit in a horizontal direction.

[0073] FIG. 10 illustrates a further embodiment for the correction of differing divergences along the fast axis and the slow axis of a laser device using optics in accordance with various implementations. In comparison to the embodiments described before, the lens array 72 is replaced by a single convergent cylindrical lens 112 that covers all lasers beams as described in FIG. 5. Diagram 107 shows a three-dimensional schematic illustration of lenses 112, 74 and 16 and scanning mirror 18A. Diagram 108 shows in the fast axis plane light beams emerging from one of the laser diodes 10B or 10R placed on the outer side through cylindrical lens 112 (preferably serves as laser window 12) and a second divergent lens 74, for instance a divergent lens as shown in FIG. 6A, where the laser diodes' tilt compensates for both lenses 112 and 74 according to the principles described in connection with FIG. 5. Diagram 110 shows, for reference, the central laser diodes' light beams co-illuminating the same scanning mirror 18A. Diagram 114 shows the slow axis orientation, in which light in this plane is refracted only by conventional lenses 16. The ellipticity of the beam in this example was reduced from 1:3.5 to an acceptable ellipticity of 1:1.5.

[0074] The configurations shown in FIG. 10 include a laser device with a 3-laser package with three laser diodes located in a same plane (shown as a single beam in diagram 114). However, another array of lasers (such as six as shown in diagram 32 or twelve shown in diagram 36) may also be implemented, in which an additional vertical tilt (as shown in FIG. 9) may be implemented if needed.

[0075] In some implementations, the laser diodes may be oriented perpendicularly so that the slow axis plane is overlapping (instead of the fast axis). In this case, the same arrangements of tilt are applicable, with the lenses at orthogonal orientations.

[0076] The distance and the lateral placement of the lens arrays 72, 72B or of single lens 112 is of great importance since misalignment can cause substantial defocusing or undesired beam shifts. FIG. 11 shows embodiments for the placement of the lens array/single lens (labelled “72/112”) in the laser package of the laser device. In diagram 116 the lens array/single lens are combined with window 12. In other words, the lens array/single lens forms the window through which the light emitted by the laser diodes exits the laser package. Frame 117 holds the lens array/single lens, thereby enabling optical power and sealing of the laser chamber of the laser package. In diagram 118 the lens array/single lens is placed directly on the submounts 26, thereby enabling a shorter optical path from the laser diodes and enabling a more accurate positioning. Diagrams 120 and 122 show the placement of the lens array/single lens facing upward or downward, respectively, on top of the submounts. A similar placement is possible where the lens array/single lens is placed on a mount (not shown) similar to submounts 26, but placed next to submounts 26, thereby enabling a stronger support while having the same accuracy since the lens array/single lens is positioned on the same base 11 as the submounts 26.

[0077] Unless otherwise stated, use of the word “substantially” may be construed to include a precise relationship, condition, arrangement, orientation, and/or other characteristic, and deviations thereof as understood by one of ordinary skill in the art, to the extent that such deviations do not materially affect the disclosed methods and systems.

[0078] The features and embodiments described in connection with the figures can also be combined with one another according to further embodiments, even if not all such combinations are explicitly described. Furthermore, the embodiments described in connection with the figures can have additional and/or alternative features according to the description in the general part.

[0079] The foregoing description of the implementations of the present disclosure has been presented for the purposes of illustration and description. It is not intended to be exhaustive or to limit the present disclosure to the precise form disclosed. Many modifications and variations are possible in light of this disclosure. It is intended that the scope of the present disclosure be limited not by this detailed description, but rather by the claims appended hereto.