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    • 专利摘要:
    A pumping device for pumping a reinforcing laser medium (1) comprises a radiation source (13) having a plurality of laser diodes (16) emitting laser beams (17) having parallel beam axes (a) extending in the direction of a z-axis and in the direction an x-axis perpendicular to the z-axis diverge at least twice as much as in the direction of a perpendicular to the z-axis and perpendicular to the x-axis y-axis, and at least one optical component (22, 22 ', 22 ") with at least a cylindrical surface (23), with which cooperates at least part of the laser beams (17) emitted by the laser diodes (16) The cylindrical surface (23) lies parallel to the x-axis and is curved in a plane perpendicular to the x-axis.
    公开号:AT513254A4
    申请号:T858/2012
    申请日:2012-08-03
    公开日:2014-03-15
    发明作者:Daniel Dr Kopf
    申请人:Kopf；
    IPC主号:
    专利说明:

    Patent Attorneys Hofmann S Fechner »· · a ♦ ♦ ♦ *
    Dr. Ralf 8ofn »ann! . * *** "*** * T (0) 5522 73 137
    Dr. Thoma »Pec!» I * er · ··· * ··· F * M3 (0) 5522 73 359 6806 Feldkirch, Austria M office@vpat.at
    Egelseestr 65a, PO Box 61 1 www.vpat.at 24388/33 / ss 120716 1
    The invention relates to a pumping device for pumping a reinforcing laser medium comprising a radiation source having a plurality of laser diodes emitting laser beams having parallel beam axes extending in the direction of a z-axis and projecting in the direction of a x axis perpendicular to the z-axis. Diverge axis at least twice as much as in the direction of a right angle to the z-axis and perpendicular to the x-axis y-axis, and at least one optical component having at least one cylindrical surface, with which cooperates at least a portion of the laser beams emitted from the laser diode.
    Recently, laser diodes have been used to pump solid-state lasers in place of conventional flash lamps. A solid-state laser pumped in this manner is described, for example, in Errico Armandillo and Callum Norrie: "Diode-pumped high-efficiency high-brightness Q-switched ND: YAG slab laser". OPTICS LEITERS, Vol. 22, no. 15.1. August 1997, pages 1168-1170. Laser diodes have particular advantages in terms of efficiency, pump efficiency and service life. In order to achieve higher pump powers, several laser diodes are combined in a common component. Barren (English "bar") are arranged on a strip-shaped chip several laser diodes (= emitter emitter) and electrically operated in parallel and mounted on a common heat sink. The individual emitters of such a bar each emit a laser beam, which in the direction of a so-called "fast-axis", which is referred to in this document as x-axis, a much larger Abstrahlwinkei than in a direction perpendicular thereto direction of a so-called "slow-axäs" ;, which is referred to in this document as the y-axis. For example, the y-direction divergence is +/- 5 ° and the divergence in the x-direction is +/- 33 °. The beam axes of the laser beams of 4 4 ··· 4 4 ··· «· 4 4 · φ · ·« · 4 t * · 2 «· ·· * · ** * ·· ··
    Laser diodes are parallel to each other and parallel to a z-axis perpendicular to the x- and y-axis.
    In laser diode stacks, which are also referred to as laser diode stack, a plurality of such bars with their broad sides and / or narrow sides are arranged side by side. A commercially available laser diode stack consists, for example, of 8 ingots arranged next to one another in the x-direction, each having 40 individual emitters spaced apart in the y direction, the emitted peak optical power being 2,400 W at a wavelength of 808 nm from an emitting surface of 10 mm × 11.9 mm , Other numbers of ingots and / or single emitters are also known.
    The laser radiation emitted by such a laser diode stack thus diverges greatly, as a result of which the imaging with optical components with which the laser radiation interacts encounters limits with regard to aperture and imaging quality. To counteract this, it is known to arrange a microlens in the form of a cylindrical lens in front of the laser diodes of a respective billet. The cylinder axes of the microlenses are aligned in the y-direction so that the strong divergence in the x-direction is reduced, e.g. below 1 °. As a result, the subsequent optics for imaging the laser radiation into the amplifying laser medium is substantially simplified. However, the use of such "fast-axis-collimation" microlenses leads to increased material and assembly costs (due to narrow tolerance requirements) and to performance losses of about 10%.
    Also known in the z-direction extending, for example, rod or truncated pyramidal optical components, of which the laser radiation is directed by total reflection to the amplifying laser medium, see. e.g. Eric C. Honea et al .: "Analysis of an intracavity doubled diode-pumped Q-switched Nd: YAG laser producing more than 100 W of power at 0.532 pm", OPTICS LEITERS, Vol. 15.1. August 1998, pages 1203 to 1205 and WO 2010/052308 A1. A disadvantage is the required length in the z-direction, which reduces the compactness of the entire laser.
    The object of the invention is to provide an advantageous pumping device of the type mentioned, which enables a compact design at a high efficiency. According to the invention, this is achieved by a pumping device having the features of claim 1.
    In the pumping device according to the invention, the cylindrical surface extends parallel to the x-axis and is curved in the y-z-plane, ie in a plane perpendicular to the x-axis. The cylindrical surface thus has an imaging, in particular collecting, effect in the y-z plane (ie with regard to the "slow-axis"), but not in the x-z plane {that is to say with regard to the "fast-axis").
    If one considers the laser radiation emitted by a respective laser diode as a laser beam with a radiation cone within which 95% of the total power of the laser radiation emitted by the laser diode, the intersecting lines of the shell of the radiation cone with a parallel zury-z plane and through The beam axis extending plane hereinafter referred to as referred to the yz plane edge rays of the laser beam. The emission angle of these marginal rays corresponds to half the total opening angle of the radiation cone in the plane lying parallel to the y-z plane and passing through the beam axis. The same applies to the marginal rays of the laser beam related to the x-z plane. The emission angle is thus the angle which a respective edge beam encloses with the beam axis, and thus defines the divergence of the laser beam emitted by the laser diode with respect to the y-z plane or with respect to the x-z plane.
    The collecting effect of the cylindrical surface in the y-z plane means that, due to the interaction with the cylindrical surface, at least divergence of the marginal rays related to the yz-plane is reduced or these marginal rays parallel to each other after interaction with the cylindrical surface (ie. ·· # ·· the opening angle of the radiation cone is zero, ie the laser beam is collimated) or even run towards each other (ie the opening angle of the radiation cone is negative).
    Preferably, for a respective laser beam, the two marginal rays related to the y-z plane subtend an angle of less than 10 ° with each other after cooperating with the cylindrical surface, i. the laser beams are at least largely collimated.
    In an advantageous embodiment of the invention, the pumping means on no reflective or refractive surface, which is only or in a plane perpendicular to the axis, ie in the xz-plane curved and with the laser beams interact with the in the yz Plane curved cylindrical surface interaction.
    The laser beams emitted by at least a plurality of laser diodes, preferably at least most of the laser diodes, particularly preferably all laser diodes, of the radiation source cooperate with this cylinder surface lying parallel to the x-axis and curved in the y-z plane, ie with the same cylindrical surface. That For the laser beams emitted by a plurality of laser diodes, preferably the majority of the laser diodes, particularly preferably all laser diodes, a common optical component having at least one such cylindrical surface is provided, with which these laser beams interact.
    In one possible embodiment of the invention, the cylindrical surface is reflective (= mirroring), so that the laser beams are reflected on the cylindrical surface (apart from losses). The cylindrical surface is concave to the side from which the laser beams are incident. In this case, in one possible embodiment, the reflection can take place on the outside of the component, without the laser beams entering the component. The component is thus formed as a cylinder mirror. In another possible embodiment variant, the laser beams can enter the component through an entry surface and be reflected on the cylinder surface in the interior of the component. The cylindrical surface can be shaped like a mirrored cylindrical surface. * 4 4 4 4 4 4 44 4444 4440 444 4 4 4 · q · · * * 4 4 4 * 4 444 ·· It is also conceivable and possible to provide a component with a mirrored inner cylindrical surface. The laser beams reflected by the cylindrical surface emerge from the component through an exit surface of the component. Preferably, the entrance surface and the exit surface are formed by different surfaces of the optical component, i. the entrance and exit surfaces are spatially separated.
    In another possible embodiment, the cylindrical surface is refractive, so that the laser beams pass through the cylindrical surface (apart from losses, in particular by reflections). It is thus the component is a cylindrical lens. The cylindrical surface may be an entry surface through which the laser beams enter the component. By means of a {= spatially separated) exit surface, which differs from the entry surface, the laser beams exit from the component again. The exit surface may be planar (= flat). The reverse design is also possible, in which the breaking cylindrical surface is the exit surface of the optical component, from which the laser beams exit from the component, wherein the entrance surface is flat (= flat). Also, both the entrance surface and the exit surface may be cylindrical surfaces that are parallel to the x-axis and curved in the y-z plane. If only the entrance surface or the exit surface is formed by such a cylindrical surface, the other of these two surfaces could also have a curved configuration in some other way, possibly only or even in the x-z plane (to also have a collection effect with respect to the x -Axis). The at least one cylindrical surface, which is curved parallel to the x-axis and curved in the y-z plane, is convex towards the outer side of the component in order to achieve a collecting effect, ie it is formed in particular by a convex surface (= outer surface) of the component
    The cylindrical surface of the optical component is formed by a part of the entire circumference of a cylinder jacket, in particular a straight cylinder, i. it represents one over a certain polar angle range < 2π • • • *
    It may be, for example, the lateral surface of a circular cylinder, parabolic cylinder or elliptical Cylinders act. Such cylindrical surfaces have a cylinder axis, which is thus parallel to the x-axis.
    The cylinder surface conveniently has a focal line (= focus line) on which rays which are parallel to an optical axis of the component coming from one side, cut or at least approximately intersect.
    In an advantageous embodiment of the invention is located in the beam path of the laser diode emitted laser beams between the laser diodes and the at least one parallel to the x-axis and in the xz plane curved cylindrical surface having optical component no other optical component with which the laser beams Interaction, ie the laser beams emitted by the laser diodes pass directly into the optical component from the laser diodes after passing through an air gap.
    The radiation source preferably comprises two or more laser diodes arranged at different locations relative to the x-axis, the laser beams of which interact with the cylindrical surface of the optical component, and particularly preferably two or more laser diodes arranged at different locations relative to the y-axis, the laser beams thereof interact with the cylindrical surface of the optical component. In an advantageous embodiment of the invention, the laser beams of all the laser diodes of the radiation source interact with the cylindrical surface of the optical component.
    Preferably, all the laser diodes of the radiation source lie in a common plane perpendicular to the z-axis (ie in an x-y plane).
    A preferred embodiment of the invention provides that the radiation source is a laser diode stack having a plurality of bars each having a plurality of laser diodes, wherein the laser diodes of a respective laser diode of a respective 7 «· * 4 # · ♦ * • ft f ··· ····· * • > »· 4 * •« · 4 4 * · ♦ * φ4 4 * ·· ## · · »
    Barrens are arranged spaced apart in the y-direction, so lie on a common, parallel zury-lying straight lines. In this case, preferably at least two ingots, in one possible embodiment of the invention, all ingots are juxtaposed relative to the direction of the x-axis, that is to say a vertical laser diode stack whose laser diodes are arranged in a plurality of y-directional rows (preferably three or more) and arranged in a plurality of columns extending in the x-direction (preferably ten or more).
    To the laser beams emitted by the laser diode in the x-direction, ie in the direction of the "fast-axis". so that the laser radiation emitted by the radiation source does not spread over an excessively large spatial area in this direction, it is advantageous if reflective boundary surfaces are provided which cover the entire extent of the laser radiation emitted by the radiation source in the direction of the x-axis on both sides limited. Of these, preferably planar {= flat) boundary surfaces, the beam portions impinging on them are reflected by the laser beams emitted by the laser diodes. The boundary surfaces are preferably at right angles to the x-axis. An advantageous embodiment provides here that the optical component, which has the at least one cylinder surface lying parallel to the x-axis and curved in the y-z plane, also has the reflective boundary surfaces. These are thus formed by side surfaces of the optical component, which are preferably perpendicular to the entrance and exit surfaces of the optical component. Conveniently, the reflection takes place at the reflective boundary surfaces by total reflection.
    It is also conceivable and possible to use separate mirrors which have the reflective boundary surfaces.
    A laser, in particular solid state laser, whose amplifying laser medium is pumped with a pumping device according to the invention is in particular pulsed. Training as a continuous wave laser is also possible. 8 ·······
    The amplifying laser medium of the laser is preferably side pumped by the pumping device. For example, it is a disk laser (= " slab laser "), e.g. Zigzag plate laser (= laser with "zig-zag slab gain medium"). The inlet and outlet surfaces of the laser medium for the laser radiation emitted by the amplifying laser medium, which is guided in the resonator of the laser, can hereby advantageously be arranged at the Brewster angle.
    Further advantages and details of the invention are explained below with reference to the accompanying drawings. In this show:
    Fig. 1 is a highly schematic representation of an embodiment of a laser pumped in accordance with the invention;
    Fig. 2 an Ausführungsbeispie! a radiation source for a pump device according to the invention, in front view;
    FIG. 3 shows the radiation source of FIG. 2 in side view; FIG.
    FIG. 4 shows the radiation source of FIG. 2 in a view from above; FIG.
    Fig. 5 is an oblique view of the radiation source of Fig. 2;
    6 shows an oblique view of a first embodiment of a pump device according to the invention in an oblique view, together with the amplifying laser medium to be pumped;
    7 shows a representation of the axial rays of the radiation beams of the individual laser diodes in the x-z plane;
    Fig. 8 is an illustration of the axial rays in the y-z plane;
    9 shows a representation of the marginal rays of the radiation cone of three of the laser diodes in a projection into the x-z plane which are related to the x-z plane and y-z plane;
    10 shows a representation of the marginal rays of the radiation cone of three of the laser diodes in a projection into the y-z plane, which are related to the x-z plane and y-z plane.
    11 to 14 representations analogous to Figures 7 to 10 for a second embodiment of the invention ..; «« * ♦
    · · · · · · · · · · · · · · · · · ·
    Figs. 15 and 16 are views similar to Figs. 9 and 10 for a third embodiment of the invention.
    The drawings have different scales. The units shown in FIGS. 7 to 16 are mm.
    A possible embodiment for a laser, which is pumped in accordance with the invention, is shown schematically in FIG. It is a solid-state laser whose amplifying (active) laser medium consists of a crystalline or glassy (amorphous) solid. For example, the reinforcing laser medium 1 may be Nd: YAG, Nd: glass, Nd: vanadate or Yb: YAG.
    The amplifying laser medium is arranged in a resonator, the components of which are explained in more detail below.
    The amplifying laser medium 1 is for example plate-shaped, that is to say a slab laser (= "slab laser"). Although the beam of the laser radiation emitted by the amplifying laser medium 1 is shown schematically running straight through the reinforcing laser medium 1 in FIG. 1, it could also run zigzag through it. The two input and output surfaces 2, 3 for the emitted laser medium 1, the resonator laser radiation passing through are advantageously arranged at Brewster angle, but this is not absolutely necessary.
    The reinforcing laser medium 1 is side-pumped, as is known. The laser radiation 5 pumping the amplifying laser medium 1 thus does not fall through the entrance and exit surfaces 2, 3 into the laser medium, but rather through a side surface 6. This is at an angle to the entry and exit surfaces 2, 3.
    The laser medium 1 could instead of plate-shaped, for example, also be rod-shaped. 10 ft ft ft ft ft ft ft ft ft ft ft ft ft ft ft
    The resonator comprises an end mirror 7 and an output mirror 8 in order to decouple the laser beam 4 emitted by the laser. The resonator shown is folded once, for which purpose a reversing prism 9 is arranged in the beam path. The folding could also be dispensed with or the resonator could be folded several times. Other folding mirrors could be provided.
    To form a Q-switch a polarizer 10, a Pockels cell 11 and a quarter-wave plate 12 are arranged in the beam path of the resonator in the illustrated embodiment. The laser radiation emitted by the laser is thus pulsed. To form pulses, other than electro-optical Q-switches, in particular acousto-optic Q-switches could be provided.
    One of the arranged in the beam path mirror, in particular the Auskoppelspiegel 8 or the final levels! As could be known, 7 could be designed as a gradient mirror, the reflectivity of which changes over the mirror surface and is greater here in a middle region than in an edge region. As a result, the beam profile of the laser beam can be influenced, for example in order to achieve a more rapid edge drop of the intensity, and / or the beam quality of the laser beam can be improved.
    The pumping of the amplifying laser medium takes place by means of a radiation source 13, which comprises a plurality of laser diodes. The optics 14 of the pumping device, in order to supply the laser radiation emitted by the radiation source advantageously to the amplifying laser medium 1, is indicated only schematically in FIG.
    The radiation source 13 is preferably designed in the form of a laser diode stack and an example of this is shown in FIGS. 2 to 5. The laser diode stack comprises a plurality of bars 15, each having a plurality of laser diodes 16 which are spaced apart in the direction of a y-axis. For example, 15 to sixty laser diodes 11 4 "9 4 * * 9 9 9 9" 9129 (= single emitter) 16 may be present per ingot. In the direction of an x-axis perpendicular to the y-axis, a plurality of such bars 15 are arranged next to one another, the laser diodes 16 being spaced from one another in the y-direction (each lying on a straight line parallel to the y-axis). For example, five to fifteen bars 15 may be present. Two or more bars 15 could also be arranged next to one another in the y-direction, so that two or more rows of juxtaposed bars 15 extending in the x-direction would be present. For one of the laser diodes 16 of the radiation source 13, the radiation cone of the laser beam 17 emitted by it is shown. The beam axis a is parallel to the z axis perpendicular to the x and y axes. The beam axes a of all laser diodes 16 of the radiation source 13 are parallel to one another, the laser diodes 16 each having the same radiation characteristic.
    A respective radiation cone of a laser diode is defined in this document in that it limits the range within which 95% of the total power of the laser radiation emitted by the laser diode is emitted.
    As referred to the x-z plane edge rays 31 of a respective one of the laser diodes are designated in this document, the lines that limit the Strahiungskegel in a section of the radiation cone with a parallel to the x-z plane and extending through the beam axis a plane. As referred to the y-z plane edge rays 31 of a respective one of the laser diodes, the lines are designated in this document, which limit the radiation cone in a section of the radiation cone with a parallel to the y-z plane and extending through the beam axis a plane.
    In other words, it could also be said that the boundary rays 31 for a respective laser diode delimit the region in a plane parallel to the x-axis and the z-axis passing through the beam axis a, within which 95% of the total power of the laser diode emitted laser radiation 12 • * * * * · 4 · * · ♦ t «· • ff I» »ffff ·· * * · emitted. In an analogous manner, the marginal rays 32 delimit such a region in a plane parallel to the y-axis and the z-axis and passing through the beam axis a.
    The radiation angle 18 related to the x-z plane is the angle between the respective edge beam 31 and the beam axis a. The radiation angle 19 related to the y-z plane is the angle between the respective edge beam 32 and the beam axis a.
    If in this document it is said that rays are shown in the x-z plane or in the y-z plane, then in each case the projection into the x-z plane or y-z plane is meant.
    The laser beams 17 emitted by the laser diodes 16 have in the direction of the x-axis at least twice as large, preferably at least three times as large, divergence as in the direction of the y-axis. Thus, the beam angle 18 related to the xz plane is at least twice as large, preferably at least three times as large as the beam angle 19 related to the yz plane. For example, the beam angle can be 18 +/- 33 ° and the beam angle 19 + / -5 °.
    The bars 15 are held on a carrier 20. In Fig. 6, a cooling body 21 is shown for cooling the laser diode stack, which may for example be water cooled (the terminals are not shown). The electronics for operating the laser diode stack is not shown in FIG. 6 for the sake of clarity.
    The pump device further comprises an optical component 22, which has a cylindrical surface 23. This is formed in this embodiment of a provided with a reflective coating outer surface of the optical component 22. The laser beams 17 emitted by the laser diodes 16 of the radiation source 13 pass through an entrance surface 24 of the optical system. 4 4 9 4 9 4 4 4. • * < * • »·· * ··· * 9 · · ·« ♦ ** * ·· Μ
    Component 22 in this (at least for the most part). After the laser beams 17 have been reflected on the cylindrical surface 23, the laser beams 17 emerge from the exit face 25 of the component 22 (at least for the most part). The entrance surface 24 and the exit surface 25 are conveniently provided with antireflection coatings.
    The exiting through the exit surface 25 laser beams reach the laser medium 1 (at least for the most part). The entrance surface 24 and the exit surface 25 are formed by different surfaces of the component 22, so do not overlap.
    In the exemplary embodiment shown, the reinforcing laser medium 1, with the side surface 6 through which it is pumped, rests directly against the exit surface 25 of the optical component 22. It could also, for example, to ensure the total reflection in a zig-zag laser, a small gap therebetween be provided or an intervening transparent material having a lower refractive index than the material of the reinforcing laser medium 1. At least the distance of the laser medium 1 from the exit face 25 measured in the direction of the surface normal to the side face 6 is advantageously smaller than the extent of the laser medium 1 measured in this direction.
    In the exemplary embodiment, the optical component 22 having the cylindrical surface 23 is the only optical component of the pumping device with which the laser radiation emitted by the radiation source 13 interacts. Preferably, at least only one optical component is present, which has an imaging, in particular collecting, effect.
    In order to allow the passage of the laser beams 17 through the component 22, this consists of a transparent material. Preferably, the transmission of the material of the optical component 22 at the wavelength of the laser beams 17 (= the wavelength of the maximum of the intensity) is more than 99%, preferably more than * * f * 4 «Μ« * * «» «*» » v 4 * * 4 * * »4« ** 44 * ·· < · * ·· * · 99.5%, over a distance of 10mm (pure material transmission, no surface reflections considered). In practical embodiments, the value may be over 99.8%. The total absorption of the laser radiation of the radiation source 13 that passes through the optical component 22 may favorably be less than 3%, particularly preferably less than 1%. The distance traveled by the laser radiation 5 can be shorter than 20 cm, preferably shorter than 10 cm. For example, the optical component may be made of glass, e.g. SF6 or SF11. Other transparent materials are also replaceable, for example YAG.
    The refractive index n of the material of the optical component 22 is greater than 1.6 in the exemplary embodiment at the wavelength of the laser radiation emitted by the radiation source 13. The refractive index of the high-index glass material SF6 is n = 1.78 at a wavelength of 808 nm.
    In other embodiments, a material with a lower index of refraction than 1.6 could also be used, e.g. a silicate glass.
    In Fig. 6 it is shown that the optical component 22 is formed of several, in particular by bonding interconnected, consisting of transparent material parts. Even a one-piece training is conceivable and possible. The optical component 22 is attached to a carrier 26. In Fig. 6, a heat sink 27 is further shown, for example, is water cooled (the terminals are not shown) and used to cool the reinforcing laser medium 1.
    If the laser beams 17 emitted by the laser diodes 16 are each understood as a beam, the axial beams 28 of the beam bundles are shown in FIGS. 7 and 8, ie the beams emitted along the beam axes a of the laser diodes 16, in FIG the x-z plane (a projection into the xz plane would be identical here) and in the yz plane in FIG. 8 (a projection into the yz plane would be identical here). FIGS. 7 and 8 thus also show the course of the curves
    • 4 4 4 ··· 444 »I optical axes of the laser beams 17 emitted by the laser diodes 16 in the x-z plane or in a projection into the xz plane and in the yz plane or in a projection into the yz Plane formed as a laser diode stack Strahiungsquelle 13, the optical component 22 and the amplifying laser medium 1 5 are shown schematically.
    The O-point of the x and y axes are placed in the center of the radiation source 13. The O-point of the z-axis is located on the surface of the radiation source 13, from which the laser radiation is emitted. 10
    With respect to the x direction, no interference of the axial rays 28 takes place through the optical component 22. The axial rays 28 run in the xz plane or in a projection onto the xz plane parallel to the z-axis from the radiation source 13 to reinforcing laser medium 1. 15
    With respect to the y-z plane, the axial rays 28, which extend parallel to one another in the z-direction up to the cylindrical surface 23, are reflected by the cylindrical surface 23 in such a way that they converge to a point. Viewed spatially, the axial beams 28 converge (at least approximately) on a cutting line parallel to the x-axis and at right angles to the y-z-plane 20, which represents the focal line of the cylindrical surface 23.
    The laser medium 1 is here arranged such that the (approximately) cut line of the axial beams 28 lies in the region of the side surface 30 facing away from the optical component 22. This side surface 30 is favorably mirrored here, so that it reflects back the laser beams 17 impinging on it. The cutting line could also be located in a middle region of the reinforcing laser medium 1 or in the region of the side surface 6. Since a contact of the side surface 6 at the exit surface 25 of the optical component 22 is preferred, the geometry of the optical component could be adapted accordingly ,
    • * * »• · · · · · · · · · · · · · · · · · · · · · · · · · · ·» t
    In FIGS. 7 and 8, the cylinder axis 29 is also shown, around which the cylindrical surface 23 is curved. For example, the cylindrical surface 23 is formed by a peripheral part of a shell of a right circular cylinder, which is curved around the cylinder axis 29. It could be e.g. also act around a curved about the cylinder axis 29 parabolic or elliptical cylinder.
    FIGS. 9 and 10 show similar representations to FIGS. 7 and 8, but here the projection of the marginal rays 31, 32 into the xz plane and into the yz plane for the laser beams 17 emitted by three of the laser diodes 16 is illustrated , These are two edge-side laser diodes 16 (of which one has the largest values of the x and y coordinates and of which the other has the smallest values of the x and y coordinates of all the laser diodes) and one with respect to the x and y-extension of the radiation source 13 located in a central region laser diode 16. Fig. 9 shows the projection in the xz plane and Fig. 10 shows the projection in the yz plane.
    Since the refractive index n of the material of the component 22 is greater than air, the angles of the marginal rays 31, 32 to the z-axis when the respective laser beam 17 enters the optical component 22 are reduced correspondingly to the ratio of the refractive indices.
    The incident on the cylindrical surface 23 marginal rays are reflected by this. With respect to the xz plane, there is no change in the divergence of the two marginal rays 31 of the laser beam 17 of a respective laser diode 16. With respect to the yz plane, the two marginal rays 32 of the laser beam 17 of a respective laser diode 16 in the embodiment after the reflection the cylindrical surface 23 in parallel. It could also be provided an education, so that the two edge beams 32 of a respective laser beam 27 converge after convergence on the cylindrical surface 23 (converge). At least the divergence of the two marginal rays 32 of a respective laser beam 17 is reduced as a result of the reflection on the cylindrical surface 23 in the y-z plane. »· · · · · · · · * *« «♦ · * · · *
    The cylindrical surface 23 thus unfolds a collecting effect for the laser beams 17 emitted by the laser diodes 16 relative to the yz plane, but not with respect to the xz plane or in other words a collecting effect with respect to the original divergence in the y direction (= in Direction of the "slow-axis") but not with respect to the original divergence in the x-direction (= in the direction of the "fast-axis").
    In this embodiment, beam portions of the laser beams 17 of the peripheral laser diodes 16 after reflection on the cylindrical surface 23 impinge on boundary surfaces 33, 34 of the optical component 22, which limit the optical component 22 in the x-direction and are preferably perpendicular to the x-axis. At these boundary surfaces 33, 34 there is a total reflection of the incident on them partial beams. The reflection is shown for the corresponding marginal rays 31 in FIG. For other than the laser beams 17 emitted by the two edge-side laser diodes, partial beams are reflected at the boundary surfaces 33, 34. Thus, the extent of the laser radiation emitted by the radiation source 13 is limited relative to the x-direction. The geometry of the arrangement could also be selected such that partial beams of laser beams 17 of the laser diodes 16 are already reflected on the boundary surfaces 33, 34 before impinging on the cylindrical surface 23.
    With reference to the x-axis, therefore, the laser radiation is guided by internal reflection at the boundary surfaces 33, 34. If the extent of the laser medium 1 in the x-axis is sufficiently large, the reflection at the boundary surfaces 33, 34 could also be dispensed with optical component 22 is then also made correspondingly long in the x-direction).
    Overall, a low-loss, largely homogeneous illumination of the laser medium 1 is achieved. Since there is a strong overlap of the laser beams 17 emitted by the individual laser diodes 16, the illumination remains • * * · · · ·······································································.
    even then relatively homogeneous, if individual of the laser diodes 16 should fail.
    The radius of curvature of the cylindrical surface 23 is for example in the range of 30mm to 100mm, in the embodiment at 57.8mm. Along the z-axis, the distance from the radiation source 13, for example, in the range between 13mm and 45mm, in the embodiment at 25mm. The tilt angle of the cylindrical surface with respect to the orientation in which the cylindrical surface intersects the z-axis is, for example, in the range of 10 ° to 25 °, in the exemplary embodiment at 15 °.
    The distance between the radiation source 13 and the cylindrical surface 23 should be such that the individual laser beams after their reflection on the cylindrical surface are at least largely collimated such that the marginal rays 32 include angles of at least less than 10 ° with each other.
    FIGS. 11 to 14 are views analogous to FIGS. 7 to 10 for a second embodiment of the invention. As an optical component 22 ', which has the cylindrical surface 23, a cylindrical mirror is provided here. The cylindrical surface 23 may for example be formed by a peripheral part of the shell of a right circular cylinder, which is curved about the cylinder axis 29, which is perpendicular to the y-z plane, that is parallel to the x-axis.
    The beam path is similar to the embodiment described above. However, it lacks the effect of reducing divergence angles upon entering a material having a refractive index greater than that of air. In order to obtain an intended width of the laser radiation in the projection onto the y-z plane at the location of the reinforcing laser medium, the cylindrical surface 23 must be curved more strongly than in the first exemplary embodiment. Overall, a less pronounced overall minimum constriction of the laser radiation results in the region in which the amplifying laser medium 1 is arranged. The, in particular spherical, aberrations with regard to the overlap of the individual beams are thus greater than in the first exemplary embodiment.
    The radius of curvature of the cylinder axis 23 may be, for example, in the range of 15mm to 30mm. The distance from the radiation source 13, measured along the z-axis, is preferably approximately in the region of half the radius of curvature (+/- 10%).
    A reflection at boundary surfaces, which limit the laser radiation with respect to the x-direction by reflection, is not shown in this embodiment. However, such a boundary could be present by providing mirrors which have such reflective boundary surfaces 33, 34. The boundary surfaces would in this case again be arranged in a plane and at right angles to the x-axis
    FIGS. 15 and 16 show illustrations analogous to FIGS. 9 and 10 or 13 and 14 for a third exemplary embodiment of the invention.
    In this embodiment, the optical component 22 "having the cylindrical surface 23 is a cylindrical lens. The cylindrical surface may be formed, for example, by a peripheral part of the shell of a right circular cylinder, which is curved about the cylinder axis 29, which is perpendicular to the y-z plane.
    The amplifying laser medium 1 is arranged here in such a way that the side surface 6, through which the laser radiation emitted by the radiation source 13 enters, lies at the location of the cylinder axis 37 relative to the z-axis. The laser medium 1 could also be arranged such that the cylinder axis 37 lies within the laser medium 1 or in the region of the rear side surface 30. The rear side surface 30 could again be formed mirrored.
    The focal length of the cylindrical lens may, for example, be in the range of 50 mm to 200 mm, the distance between the cylindrical lens and the 20 * * 20 * * * * * · * • * * * * · * * * * 4 * · «· · ·« · «Μ · ·
    The range between the cylindrical lens and the laser medium 1 is also within the range of the focal length (+/- 10%).
    After passing through the optical component 22 " The two edge beams 32 of the laser beam 17 of a respective laser diode 16 preferably run together or parallel to each other. At least the divergence of the two marginal rays 32 from the optical component 22 " reduced. The optical component 22 " thus has a collecting effect relative to the original divergence in the y-z plane.
    With respect to the x-z plane, the divergence of the two marginal rays 31 of the laser beam 17 of a respective laser diode 16 is not reduced. In the exemplary embodiment, however, plane mirrors 35, 36 are provided whose mirror surfaces form boundary surfaces 33, 34 for the laser radiation, wherein the boundary surfaces 33, 34 are at right angles to the x-axis. The extension of the laser radiation of the laser radiation emitted by the radiation source 13 in the x-direction is thereby limited again.
    If the extent of the laser medium 1 in the x-direction is sufficiently large, the boundary surfaces 33, 34 could in turn be omitted.
    The individual laser beams 17 of the laser diodes 16 overlap well in the region of the laser medium 1. In view of the relatively large focal length, however, the area illuminated by the laser radiation is relatively large, and the amplifying laser medium 1 must be correspondingly large.
    Advantageously, the focal length of the cylindrical lens is more than five times the relative to the direction of the y-axis distance between the two in the y-direction the greatest distance from each other having laser diodes of the radiation source.
    ·······················································.
    The use of cylindrical lenses with shorter focal lengths is possible, but this is accompanied by a reduction in the collimation and the homogeneity of the illumination. 5 The cylindrical surface of the component 22 " could also be arranged on the laser medium 1 side facing. A cylindrical lens with double-sided cylindrical surfaces could also be used.
    By means of a pump device according to the invention, it is possible in particular to provide compact 10 side-pumped solid-state lasers. For example, a laser with at least 100 mj of pulse energy and pulses shorter than 20 ns can be realized. The "foot print" (= Laser head without electronics) may have dimensions of less than 15cm x 10cm, preferably dimensions in the range of 10cm x 5cm, and have less than 2kg mass, so it is suitable for "hand held" -15 applications.
    On the other hand, a pulsed laser with greater than 3 mJ pulse energy and less than 10 ns pulse length can be provided, having dimensions of less than 10 cm x 5 cm or even less (again laser head, without electronics). By the invention, a compact pulse laser can be provided which has a high efficiency of more than 10% or even more than 15% with respect to the energy of the generated pulse in relation to the energy of the (optical) pumping pulse. Due to the efficiency, a compact pulse laser may be provided if necessary, which does not require water cooling. Optionally, a 100 Hz / 100 mJ laser can be provided which is suitable for battery operation in practice.
    In particular, the use of a cylindrical surface cylindrical lens with a long focal length, e.g. shown in the third embodiment of the invention, for the pumping of a laser with a high energy, in particular 1 J or more advantageous. 30 22 ·································································································································· · ♦ ♦
    A pumping device according to the invention could also be used for pumping other than the mentioned solid-state lasers, for example also for
    Pumping fiber or disk lasers. A device according to the invention also has the advantage that the positional and angular tolerances of the radiation source, in particular in the form of a laser diode stack, are relatively uncritical in comparison with the prior art. Thereby, e.g. the radiation source, in particular in the form of a laser diode stack, be provided as a user replaceable module. 10 * · 23 * »» * ♦ * ··
    Key to the reference numbers: 1 amplifying laser medium 19 radiation angle 2 entrance surface 20 support 3 exit surface 21 heat sink 4 laser beam 25 22, 22 ', 22 " optical component 5 laser radiation 23 Zyiinderf pool 6 side surface 24 entrance surface 7 end mirror 25 exit surface 8 Auskoppelspiegel 26 support 9 reversing prism 30 27 heat sink 10 polarizer 28 axial beam 11 Pocke Is-Ze Ile 29 cylinder axis 12 Lamda quarter platelets 30 side surface 13 radiation source 31 edge beam 14 Optics 35 32 Border beam 15 Bar 33 Boundary surface 16 Laser diode 34 Boundary surface 17 Laser beam 35 Mirror 18 Radiation angle 36 Mirror
    权利要求:
    Claims (11)
    [1]
    V Patent Attorneys • · · · t 4 · · · Hofmann & Fechner Ralf Hc ^ fmajjifJ '# Dr. Thomas T% chn% T * 0806 Feldkirch, Austria. ΐ * 43 «0) 5522 73 137 ..... F 43 (0) 5522 73 359 Egelseestr 65a, PO Box 61 M office@vpat.at I www.vpat.at 24388/33 / ss 120713 1. 5 10 2 A pumping device for pumping a reinforcing laser medium (1), comprising a radiation source (13) having a plurality of laser diodes (16) which emit laser beams (17) which are parallel, in the direction of a z-axis extending beam axes (a) and diverge at least twice as much in the direction of a perpendicular to the z-axis x-axis as in the direction of a right angle to the z-axis and perpendicular to the x-axis y-axis, and at least one optical component ( 22, 22 ', 22 ") having at least one cylindrical surface (23) with which cooperates at least part of the laser beams (17) emitted by the laser diodes (16), characterized in that the cylindrical surface (23) is parallel to the x-axis and is curved in a plane perpendicular to the x-axis. Pumping device according to claim 1, characterized in that the radiation source (13) comprises two or more with respect to the x-axis arranged at different locations laser diodes (16) whose laser beams (17) with the cylindrical surface (23) cooperate. Pumping device according to claim 1 or 2, characterized in that the radiation source (13) comprises two or more relative to the y-axis arranged at different locations laser diodes (16) whose laser beams (17) with the cylindrical surface (23) cooperate. Pumping device according to one of Claims 1 to 3, characterized in that the laser beams (17) of all the laser diodes (16) interact with the cylindrical surface (23) of the optical component (22, 22 ', 22 "). ia ft «· *» · · * · · «······ k · · * · · · · · i: i · μ« * · «· • ·« * · IM • ·
    [2]
    5. Pumping device according to one of claims 1 to 4, characterized in that the cylindrical surface (23) of the component (22, 22 ', 22 ") has a collecting effect on the cooperating with the cylindrical surface (23) laser beams (16)
    [3]
    Pumping device according to claim 1 to 5, characterized in that the optical component (22 ") is a cylindrical lens.
    [4]
    7. Pumping device according to claim 1 to 5, characterized in that the optical component (22 ') is a cylindrical mirror 10th
    [5]
    8. Pumping device according to claim 1 to 5, characterized in that the optical component (22) has an inlet surface (24) through which the laser of the laser diode (16) emitted laser beams (17) or at least a part thereof in the optical component (24). 22) and through the optical component (22) to the reflective 15 formed cylindrical surface (23) of the optical component (22) and from there through the optical component (22) to an exit surface (25) of the optical component (22) and through this to amplifying laser medium (1) pass or arrive, wherein the entrance surface (24) and the exit surface (25) of different surfaces of the optical component (22) are formed. 20
    [6]
    9. Pumping device according to one of claims 1 to 8, characterized in that the pumping means has reflective boundary surfaces (33, 34) which limits the extent of the radiation source (13) emitted laser radiation in the direction of the x-axis on both sides. 25
    [7]
    10. Pumping device according to claim 8 and claim 9, characterized in that the optical component (22) has the boundary surfaces (33, 34).
    [8]
    11, pumping device according to one of claims 1 to 10, characterized in that the radiation source (13) is a laser diode stack having a plurality of bars (15) each having a plurality of laser diodes (16). 3 12. * 9 ** 999 «99t *« 9t »• • 9 9 9 9 • * 9 9 9 9 9 9 9 * 9 9 9 · 9 * 9 9 * · 9 9 9 9 9 9 •« t * Pumping device according to claim 11, characterized in that the laser diodes (16) of a billet (15) are arranged spaced apart in the direction of the y-axis.
    [9]
    13. A pumping device according to claim 12, characterized in that all the bars (15) or at least a part of the bars (15) are arranged side by side with respect to the direction of the x-axis.
    [10]
    14. A laser comprising a solidifying medium formed by a solidifying laser medium (1) 10 and a pumping device for pumping the reinforcing laser medium (1), characterized in that the pumping device is designed according to one of claims 1 to 13.
    [11]
    15. A laser according to claim 14, characterized in that the reinforcing laser medium (1) is side pumped. 15
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    同族专利:
    公开号 | 公开日
    EP2880723B1|2017-05-03|
    CN104521076B|2017-12-01|
    WO2014019003A1|2014-02-06|
    US9306365B2|2016-04-05|
    CN104521076A|2015-04-15|
    AT513254B1|2014-03-15|
    EP2880723A1|2015-06-10|
    US20150244141A1|2015-08-27|
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    法律状态:
    优先权:
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    ATA858/2012A|AT513254B1|2012-08-03|2012-08-03|Pumping device for pumping a reinforcing laser medium|ATA858/2012A| AT513254B1|2012-08-03|2012-08-03|Pumping device for pumping a reinforcing laser medium|
    CN201380041314.XA| CN104521076B|2012-08-03|2013-07-26|Pump arrangement for pumping laser gain media|
    EP13756283.1A| EP2880723B1|2012-08-03|2013-07-26|Pumping device for pumping an amplifying laser medium|
    PCT/AT2013/000126| WO2014019003A1|2012-08-03|2013-07-26|Pump device for pumping an amplifying laser medium|
    US14/418,983| US9306365B2|2012-08-03|2013-07-26|Pump device for pumping an amplifying laser medium|
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