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    • 专利摘要:
    A solid-state laser has a reinforcing laser medium (1) for generating a laser beam (4) and a pump device (13, 14) having at least one laser diode (16), from which a pump radiation (5) is generated which is directed onto a first side surface (6 ) of the laser medium (1), which is parallel to a z-axis and parallel to a right-angled to the z-axis y-axis. On one of the first side surface (6) opposite the second side surface (23), the laser medium (1) is cooled by a heat sink (22). The length of a y-1 / e2 region (33) of the pump radiation (5) is smaller than the length of the first side surface (6) of the laser medium (1) in the y-axis direction, the y-1 / e2 region (33) of the pump radiation (5) denotes a section of the y-axis, via which the intensity of the pump radiation (5) on the first side surface (6) of the laser medium (1) has a value which is more than the maximum intensity of the pump radiation ( 5) on the first side surface (6) of the laser medium (1) divided by e2. The length of a y-cooling region (26), which denotes a portion of the y-axis over which a cooling strip (24) extends, is less than 70% and greater than 50% of the length of a y-pumping region (28) of the laser medium (1), wherein the y-pumping region (28) denotes a section of the y-axis, over which 80% of the total absorbed by the laser medium (1) power of the pump radiation (5) is absorbed and at both ends of the intensity of the pump radiation ( 5) is the same size. (Fig. 4)
    公开号:AT515674A4
    申请号:T184/2014
    申请日:2014-03-14
    公开日:2015-11-15
    发明作者:Daniel Dr Kopf
    申请人:Daniel Dr Kopf；
    IPC主号:
    专利说明:

    The invention relates to a solid-state laser with a reinforcing laser medium for generating a laser beam and at least one laser diode having pumping device, from which a pump radiation is generated which impinges on a first side surface of the laser medium, which is parallel to a z-axis and parallel to a is perpendicular to the z-axis y axis, viewed in a direction perpendicular to the z-axis and perpendicular to the y-axis x-axis, the laser beam parallel to the z-axis through the laser medium, wherein the laser medium at a cooled parallel to the z-axis and lying parallel to the y-axis and the first side surface second side surface by a heat sink with which it is in thermal communication, wherein the length of a y-cooling region is smaller than the length of the second side surface of the laser medium in Direction of the y-axis, wherein the y-cooling region of the laser medium ei denotes a portion of the y-axis, over which extends a cooling strip, via which the laser medium on the second side surface is thermally connected to the heat sink, wherein the length of a y-1 / e2 region of the pump radiation is smaller than the length of the first side surface the laser medium is in the y-axis direction and the first side surface of the laser medium extends beyond the y-1 / e2 region of the pump radiation in both y-axis directions, the y-1 / e2 region of the pump radiation being a portion the y axis through which the intensity of the pump radiation at the first side surface of the laser medium has a value which is more than the maximum intensity of the pump radiation at the first side surface of the laser medium divided by e2.
    Side-pumped solid-state lasers, especially those with a zig-zag geometry (= laser with "Zig-Zag slab gain medium"), are widespread. Nd: YAG is the best-known laser medium for nanosecond lasers due to the relatively high
    Gain, a storage time of 250 ps and availability in large slabs (> 10 cm) at comparatively low cost. In addition to Nd: YAG are as reinforcing laser media (= laser-active materials) u.a. Nd: glass, Nd: VANADAT or Yb: YAG known.
    For pumping solid state lasers laser diodes are used more recently instead of flash lamps. For example, a solid state laser pumped in this manner is described in Errico Armandillo and Callum Norrie: "Diode-pumped high-efficiency high-brightness Q-switched ND: YAG slab laser", OPTICS LETTERS, Vol. 15, August 1, 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 (= single 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". a significantly larger emission angle, e.g. +/- 33 °, than in a direction perpendicular thereto of a so-called "slow-axis", in which the emission angle is e.g. +/- 5 °. 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. In order to supply the laser radiation emitted by such a laser diode stack, which strongly diverges, bundled correspondingly to the amplifying laser medium, different types of optical systems have been used. For example, it is known to arrange a microlens in the form of a cylindrical lens in front of the laser diodes of a respective ingot, the cylinder axes being directed in the direction of the "slow-axis". aligned so that the strong divergence towards the "fast-axis" 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.
    From WO 2014/019003 A1 it is known to use a common cylindrical mirror, whose cylinder axis in the direction of the "fast axis". is aligned and the light of all the laser diodes in the direction of the "slow axis". bundles, or to use such a cylindrical lens. In this case, a high pumping efficiency can be achieved with a compact design.
    Various other optical systems for bundling the light emitted from laser diode bars, e.g. for pumping solid-state lasers are known, for example from US 2011/0064112 A1, US 2007/0064754 A1 or JP P2004-96092 A.
    A problem with solid-state lasers is thermal effects that lead to the formation of thermal lenses and / or to the generation of stress-induced birefringence. For example, Nd: YAG shows relatively strong such thermal effects. Stress-induced birefringence, especially in radially symmetric pump geometries, e.g. in the formation of the laser medium in the form of a cylindrical rod, a polarization rotation of parts of the beam profile and subsequently to a loss of a polarizing element in the resonator, resulting in active Q-switching with electro-optical elements (Pockels cells) to a significant loss can lead. This effect of stress-induced birefringence is minimized or almost absent in the zig-zag plate laser. The formation of a thermal lens can also be minimized in the plane of the zigzag-shaped course of the laser beam (xz-plane) in the zig-zag disk laser, but in the direction perpendicular thereto (direction of the y-axis) results in a not disappearing positive thermal lens. This makes it necessary to install compensating optics, which then have a compensating effect only for a specific power range. With an Nd: YAG laser, this is already required from about 1 watt average output power, depending on the requirements of beam symmetry and astigmatism.
    A solid-state laser of the type mentioned at the beginning is Donald B. Coyle et al .: "Efficient, reliable, long-lifetime, diode-pumped Nd: YAG laser for space-based vegetation topographical altimetry", APPLIED OPTICS, Vol. 27, September 20, 2004, pages 5236-5242. The laser medium, which is in the form of a "slab", that is to say prismatic, has a longitudinal axis which extends in the direction of a z-axis and has side surfaces which are parallel to orthogonal and perpendicular to the z-axis. and y-axes are. The laser beam passes through the laser medium zig-zag in the x-z plane. The pumping by means of laser diodes is effected by a parallel to the y- and parallel to the z-axis first side surface and the laser medium is cooled at the opposite and lying parallel to the first side surface second side surface. In order to achieve a more uniform temperature distribution in the laser medium, whereby the thermal lens with respect to the y-direction can be reduced, the cooling is not over the entire extent of the second side surface in the direction of the y-axis but only over a strip with a reduced contrast Width in the direction of the y-axis. This is achieved by a step of the voltage applied to the second side surface heatsink. However, there is still the formation of a, albeit reduced, thermal lens, which is compensated by the use of a negative cylindrical lens in the resonator.
    The incident on the first side surface pump radiation has a substantially gauss-shaped profile in this laser. Considering the two points at which the intensity of the pump radiation with respect to the y-axis has fallen to a value of 1 / e2 of the maximum intensity, the length of this y-1 / e2 region of the pump radiation is smaller than the length the first side surface of the laser medium in the direction of the y-axis. The laser medium is thus pumped with respect to the y-direction is not substantially uniform to its edge but only in a more or less central area. This has the consequence that the limited extent of the laser medium in the y-direction does not act as an aperture for the laser radiation. If, on the other hand, the laser medium were pumped over its entire extent in the y-direction, then the formation of a thermal lens in the y-direction could be substantially avoided, but the aperture then caused by the laser medium in the y-direction would have a negative effect on the quality of the laser laser beam emitted by the solid-state laser.
    The object of the invention is to provide an improved solid state laser of the type mentioned. According to the invention, this is achieved by a solid-state laser having the features of claim 1.
    In the solid-state laser according to the invention, the length of a y-cooling region of the laser medium is less than 70% and greater than 50% of the length of a y-pumping region of the laser medium, with the y-pumping region extending in both y-axis directions beyond the y-cooling region extends. As already mentioned, the y-cooling region of the laser medium denotes a section of the y-axis, over which a cooling strip extends, via which the laser medium is connected to the heat sink. The y-pumping region of the laser medium denotes a section of the y-axis, over which 80% of the total absorbed by the laser medium power of the pump radiation is absorbed and at both ends of the intensity of the pump radiation is equal. Thus, the majority of the heat is introduced into the laser medium via the y-pumping region.
    It has been found that with such a design of a solid-state laser, a thermal lens in the y-direction can be at least largely or completely avoided. This can be explained by a central depression in the temperature distribution, as will be explained in more detail below. In particular, this succeeds in conjunction with a beam profile of the pump radiation, which is more likely than in the direction of a Gaussian profile in the direction of a rectangular beam profile.
    That the profile of the pump radiation is more rectangular than Gaussian means that advantageously in the solid state laser according to the invention the difference between the length of the y-1 / e2 region of the pump radiation and the length of a y-valued region of the pump radiation is less than half is great as the difference between the length of a y-1 / e2 region and the length of a y-valued region of an imaginary ray of the same wavelength having a Gaussian profile and of which the length of a y-half-value region is equal to the length of the y y half-power range of the pump radiation and its radiation energy is equal to the radiation energy of the pump radiation. As already mentioned, the y-1 / e2 region of the pump radiation designates a section of the y-axis, via which the intensity of the pump radiation at the first side surface of the laser medium has a value which is more than the maximum intensity of the pump radiation at the first Side surface of the laser medium divided by e2, that is more than about 13.5%. The y half-value region of the pump radiation designates a section of the y axis over which the intensity of the pump radiation at the first side surface of the laser medium has a value that is more than half the maximum intensity of the pump radiation at the first side surface of the laser medium. Analogously, the y-1 / e2 range and the y-half-value range of the imaginary Gaussian beam are defined.
    This means that the pump radiation has a much stronger edge drop than is the case with a Gaussian profile. The pump radiation is thus more approximate to a Gaussian profile to a rectangular profile.
    In particular, according to the invention, an advantageous solid-state laser can be formed in which the laser beam (= the laser mode) runs zigzag through the laser medium, in a plane perpendicular to the y-axis.
    For example, a laser can be provided which emits a substantially symmetrical beam in a power range from 0 to more than 5 W average power. In particular, over the entire power range, a beam with a beam divergence of <250prad (half-angle divergence) in both transverse directions and a quality factor ΜΛ2 of <5, preferably <3, can be achieved.
    By way of example, a pulsed solid-state laser, in particular Nd: YAG Zig-Zag laser, with> 50mJ energy and a beam with low beam divergence (eg <250prad half-angle divergence) and good beam quality (eg MA2 <5 or <3), regardless of the repetition rate, eg both in single pulse mode (singleshot) and at 50Hz or 100Hz (corresponding to 5W average power) the narrowly defined beam parameters are met.
    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 according to the invention;
    2 shows an oblique view of the pumping device and the laser medium and the heat sink in greater detail;
    3 is an oblique view of the radiation source of the pumping device;
    4 shows a section through the laser medium and a part of the pumping device and the heat sink in the y-x-plane (section line AA of Fig. 5).
    Fig. 5 is a side view of the laser medium and a part of the heat sink and the pumping means in the direction of the y-axis (viewing direction B in Fig. 4).
    6 shows a side view of the laser medium on the pumped first side surface in the direction of the x-axis (viewing direction C in FIG. 4), wherein a "pumped region" is shown in FIG. illustrated by a hatching and the voltage applied to the opposite second side surface cooling strip is shown in dashed lines;
    7 shows a diagram for the comparison of the intensity distribution of the pump radiation on the first side surface of the laser medium with respect to the y direction in comparison to the intensity distribution of an imaginary beam with a Gaussian profile;
    Fig. 8 is a diagram in which the refractive index D of the formed thermal lens with respect to the y-direction in dependence on the length of the y-cooling region is shown.
    A possible embodiment of a solid-state laser according to the invention is shown schematically in FIG. It is a solid-state laser whose amplifying (active) laser medium 1 consists of a crystalline or glassy (amorphous) solid. For example, the amplifying laser medium may be Nd: YAG, Nd: glass, Nd: vanadate, Yb: YAG, Er: YAG or Ho: YAG.
    The amplifying laser medium 1, which can also be referred to as a laser-active material, is arranged in a resonator, the components of which are explained in more detail below.
    The amplifying laser medium 1 is formed prismatic, so it is a disk laser (= "slab laser"). Although the laser beam 4 formed by the emission of the amplifying laser medium 1 is shown running zig-zag through the amplifying laser medium 1 in FIG. 1, it could also be straight therethrough. The inlet and outlet surfaces 2, 3 for the emitted laser medium 1, the resonator passing through the laser beam 4 are advantageously arranged at Brewster angle, but this is not absolutely necessary.
    The reinforcing laser medium 1 is side-pumped, as is known. The pumping radiation 5 pumping the amplifying laser medium 1 thus does not enter the laser medium through the input and output surfaces 2, 3, but rather through a first side surface 6. The latter is at an angle to the input and output surfaces 2, 3. In particular, the pump radiation 5 hits at least substantially centrally on the first side surface 6.
    The resonator comprises an end mirror 7 and a coupling-out mirror 8 in order to couple out the laser beam 4a emitted by the laser. The illustrated resonator is folded once, for which purpose a reversing prism 9 is arranged in the beam path. The folding could also be omitted 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 beam 4a emitted by the laser is thus pulsed. To form pulses, for example, 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 end mirror 7 is preferably formed as known as a gradient mirror whose reflectivity changes over the mirror surface and this is greater in a central 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 pumping device which has 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 13 advantageously to the amplifying laser medium 1, is indicated only schematically in FIG.
    The radiation source 13 is preferably in the form of a laser diode stack and an example of this is shown in FIG. The laser diode stack comprises a plurality of adjacent bars 15, each having a plurality of laser diodes 16 spaced apart in one direction.
    The rays 17 emitted by the laser diodes 16 have in the direction of an axis perpendicular to the beam axis of the respective beam 17, which is referred to as "fast-axis". is more than three times as large as divergence in the direction perpendicular to the beam axis and perpendicular to the "fast-axis". standing axis, called "slow-axis". referred to as. For example, the radiation angle (= the divergence) with respect to the "fast-axis" can be used. +/- 33 ° (ie 66 ° opening angle of the radiation cone) and the angle of radiation with respect to the "slow-axis". +/- 5 °.
    The bars 15 are held on a carrier 20, cf. Fig. 2, which is mounted on a, for example, water-cooled, heat sink 21.
    The optics 14 of the pumping means is formed in the embodiment of an optical component having a reflective cylindrical surface 14b, at which the emitted from the laser diode 17 of the radiation source and entering through the entrance surface 14a in the optical component beams are reflected. This cylindrical surface 14b in this case has a collecting effect with respect to the "slow-axis". Regarding the "fast-axis" If the divergence of the beams 17 remains, only reflection or multiple reflections occur at side surfaces 14c of the optical component in order to limit the range of the radiation in this direction.
    The optical component forming the optics 14 of the pump device can be formed, for example, as shown in FIG. 2, from a plurality of parts connected to one another by bonding and made of transparent material. The optical component is attached to a carrier 18.
    Through the exit surface 14d, which is here separated by a small gap from the laser medium 1 to ensure the total resection of the laser beam 4 in the laser medium at its zigzag-shaped course, the radiation emitted by the pumping device reaches the first side surface 6 of the laser medium as pumping radiation 1.
    Such a pumping device is known from WO 2014/019003 A1 mentioned in the introduction to the description. A use of a pumping device with optics, which has a cylindrical mirror or a cylindrical lens, wherein the cylinder axis in the direction of the "fast axis". is aligned, is advantageous. For pumping the laser medium 1 pumping devices designed in a different way could also be used.
    The first side surface 6 of the laser medium 1, through which the pump radiation 5 enters, is parallel to the z axis and parallel to the y axis, ie parallel to the y z plane.
    In particular, the z-axis forms the longitudinal axis of the laser medium 1.
    The zigzag-shaped course of the laser beam 4 through the laser medium 1 lies in a plane which is parallel to the x-axis and parallel to the z-axis, ie parallel to the x-z plane.
    Viewed in the direction of the x-axis, ie with respect to the projection into the y-z plane, the laser beam 4 (= the laser mode) runs in the direction of the z-axis through the laser medium 1 (= parallel to the z axis).
    The x, y, and z axes form a Cartesian coordinate system.
    The laser medium 1 is cooled by a heat sink 22. The cooling takes place on a second side surface 23 of the laser medium 1, which is parallel to the first side surface 6, that is also parallel to the y-z plane. For this purpose, the second side surface 23 is connected to the heat sink 22. The connection to the heat sink 22 is made via a cooling strip 24. In addition, there is preferably an optical coating (not shown in the figures) on the second side surface 23 of the laser medium 1. This is applied to the second side surface 23 to ensure that, on the one hand, the total reflection of the zigzag-guided laser beam is maintained and, on the other hand, the remaining pump radiation is reflected back into the crystal and does not impinge on the cooling strip 24. Such coatings are quite common in page-pumped zig-zag lasers. In addition, for attaching the cooling strip 24 to the second side surface 23 of the laser medium 1 or the optical coating applied thereon, it is favorable to provide a bonding material (in particular, an adhesive or a solder). The cooling strip 24 consists here of a material differing from the laser medium 1 and heat sink 22 material, which over the
    Connecting material on the second side surface 23 of the laser medium 1 or the optical coating applied thereto is applied. The cooling strip 24 could also be formed by a strip-shaped elevation of the heat sink 22 and would thus consist of the same material from which the remaining heat sink 22 is made. Also in this case, the cooling strip could be applied directly or via a connecting material (in particular an adhesive or a solder) to the laser medium 1 or the optical coating applied thereto.
    The thermal conductivity of the material of the cooling strip 24 is preferably greater than 5 W / mK. Away from the region over which the cooling strip 24 extends, the second side surface 23 is separated from the heat sink 22 by an air gap 25. In this area, instead of the air gap, a solid material could also be provided, at least regionally, which has a thermal conductivity that is less than half the thermal conductivity of the material of the cooling strip 24.
    Preferably, the thermal conductivity of the material present outside the cooling strip 24 between the laser medium 1 and the heat sink 22 (which may in particular be gaseous or solid) is less than 2 W / mK, more preferably less than 1 W / mK.
    The second side surface 23 faces the first side surface 6, i. When viewed in the direction of the x-axis, the side surfaces 6, 23 overlap at least partially, preferably at least for the most part (i.e., over more than 50% of their areas).
    It is preferable that the first and second side surfaces 6, 23 extend over the same range with respect to the direction of the y-axis.
    The laser medium 1 preferably has a prismatic shape. The base and top surfaces 37, 38 are conveniently parallel to the x-z plane, which is a straight prism, in particular a parallelepiped.
    For example, the extension of the laser medium 1 relative to the y-direction is 5 mm to 15 mm, in the exemplary embodiment 8 mm. The extension of the laser medium in the x direction is, for example, 2 mm to 8 mm, in the exemplary embodiment 4 mm. The extension of the laser medium in the z-direction is for example 20mm to 80mm, in the embodiment about 40mm.
    The cooling strip 24 is for example replaced by a graphite foil, e.g. Formed 125 pm or 250 pm thick. The heat conduction of such a graphite foil can be for example 16 W / mK. The connection of the graphite foil to the second side face 23 of the laser medium 1 and the heat sink 22 can be effected for example by gluing and / or jamming. In another possible embodiment, the cooling strip 24 is formed by an indium strip. Such an indium strip can, for example, be soldered to the second side face 23 of the laser medium 1 and the heat sink 22. The solder is indium or AgSn (e.g., 96.5% Sn and 3.5% Ag) or the harder AuSn.
    For example, the heat sink 22 may be made of copper tungsten having a coefficient of thermal expansion similar to Nd: YAG, e.g.
    Copper tungsten with 85% W and 15% Cu.
    Other materials for the cooling strip 24 and / or the heat sink 22 are conceivable and possible. For example, the cooling strip 24 could also be formed by a strip-shaped elevation of the heat sink 22, which is in thermal contact with the second side surface 23 of the laser medium 1, for example by being pressed or soldered to the second side surface 23.
    The cooling strip 24 extends in the y-direction over a portion 26 of the y-axis, which is referred to in this document as the y-cooling region. Furthermore, the cooling strip 24 extends with respect to the z-direction over a portion 27 of the z-axis, which is referred to in this document as the z-cooling region.
    In this document, a y-pumping section 28 is referred to as the y-pumping region, via which 80% of the total power of the pumping radiation absorbed by the laser medium 1 is absorbed. The y-pumping region 28 is selected so that the intensity of the pumping radiation 5 at the two ends of the y-pumping region is the same. Furthermore, in this document, the z-pumping area is the section 29 of the z-axis, via which 80% of the total absorbed by the laser medium 1 power of the pump radiation 5 is absorbed. In this case, the z-pumping region 29 is selected so that the intensity of the pumping radiation is the same at both its ends. The y and z pumping areas are illustrated in FIG. 6 by a hatched area. The part of the volume of the laser medium 1 forming a cube, of which opposite side surfaces are formed by those parts of the first and second side surfaces 6, 23 of the laser medium 1, which are covered by the hatched area in FIG Font as "pumped volume &quot; of the laser medium 1. In the pumped volume of the laser medium 1 is thus the main part, namely 80%, the absorption of the power of the pump radiation, so that also introduced according to the main part of the heat introduced by the pump radiation heat in the pumped volume of the laser medium 1. Accordingly, the excitations of the laser medium 1 to the inversion level mainly, namely to 80%, in the pumped volume. The pumped volume can thus be determined from the inversion density.
    The inversion density can be measured in particular by fluorescence images. For example, for this purpose, the heat sink 22 can be removed and the recording of fluorescence images by the second side surface 23 take place, wherein the pump radiation 5 is shielded by a filter.
    The pumped volume thus extends in the direction of the x-axis over the extent of the laser medium 1. In the direction of the z-axis, the extent of the pumped volume is preferably more than 50% of the extension of the laser medium 1 in the z-axis direction and less than 90 % of the extension of the laser medium 1 in the direction of the z-axis.
    In the direction of the y-axis, the extent of the pumped volume is preferably in the range of one third to two thirds of the extent of the laser medium 1 in the direction of the y-axis.
    The pumped volume is preferably in a central region of the laser medium 1 relative to the direction of the z-axis and to the direction of the y-axis.
    The incident on the first side surface 6 pump radiation 5 has a relation to a beam with a Gaussian distribution substantially closer to a rectangular profile intensity distribution. FIG. 7 shows the distribution 35 of the intensity I of the pump radiation with respect to the y-axis. The maximum value of the intensity is lr The zero point of the y-axis is placed at the position of the maximum value of the intensity. For comparison, the distribution 36 of the intensity of an imaginary beam of the same wavelength is plotted with a Gaussian profile having the same half-width, the maximum value of the intensity being at the zero point of the y-axis. The maximum value of the intensity here is l2. The radiation energy of the imaginary beam, ie the area enclosed by the distribution 36, is equal to the radiation energy of the pump radiation.
    The section 31 of the y axis, via which the intensity of the pump radiation 5 is more than half the maximum intensity of the pump radiation at the first side surface of the laser medium 1, is referred to in this document as the y half-value region of the pump radiation. The length of this section 31 thus corresponds to the half-width of the intensity profile of the pump radiation 5. Analogously, the half-power range of the imaginary beam is defined and the corresponding section of the y-axis which coincides with the section 31 is indicated in FIG 32 denotes.
    In Fig. 7, the locations on the y-axis are further indicated at which the intensity of the pump radiation 5 and the imaginary beam has dropped to a value which is 1 / e2 (ie about 13.5%) of the maximum value. The y-1 / e2 region of the
    Pump radiation 5 correspondingly designates the section 33 of the y-axis, via which the intensity of the pump radiation at the first side surface 6 of the laser medium 1 has a value which is more than the maximum intensity of the pump radiation at the first side surface 6 of the laser medium 1 divided by e2 , Similarly, the y-1 / e2 region of the imaginary ray is defined, and the corresponding portion of the y-axis is designated by reference numeral 34 in FIG.
    The difference between the length of the y-1 / e2 region 33 of the pump radiation 5 and the length of the y half-value region 31 of the pump radiation 5 can be read off from FIG. 7 for the present exemplary embodiment by approximately 0.85 mm. The difference between the length of the y-1 / e2 region 34 and the length of the y-half-value region 32 of the imaginary beam with the Gaussian profile can be read off from FIG. 7 at approximately 2.6 mm. This difference is thus less than half as large for the pump radiation 5 as for the imaginary beam with the Gaussian profile.
    Furthermore, the length of the y-1 / e2 region 33 of the pump radiation 5 is smaller than the length of the first side surface 6 of the laser medium 1 in the direction of the y-axis, with the first side surface 6 of the laser medium 1 moving in both directions of the y axis. Axis extending beyond the y-1 / e2 region of the pump radiation, preferably the same distance. For example, the length of the y-1 / e2 region 33 of the pump radiation 5 is 4 mm, while the length of the first side surface 6 of the laser medium 1 in the direction of the y-axis is 8 mm.
    As can be seen from FIG. 6, the length of the y-cooling region is smaller than the length of the laser medium 1 in the direction of the y-axis. However, the length of the y-cooling region is also smaller than the length of the y-pumping region, as will be explained below.
    In FIG. 8, measured values are plotted as black squares, which reflect the dependence of the refractive power D of the formed thermal lens as a function of the length I of the y cooling range. If the y-cooling area extends over the entire y-dimension of the laser medium 1, then the refractive power of the thermal lens with respect to the y-direction with the operating parameters used in the test arrangement is above 1m'1. As the y-cooling range is reduced, the refractive power initially decreases slowly, and at a length I of the y-cooling region of 3 mm, which is thus significantly smaller than the length of the y-pumping region of 4 mm, to a value of just under 0.5 m '1 has dropped. In a further reduction of the length I of the y-cooling region, the refractive power of the thermal lens further decreases and is already negative at a length I of the y-cooling range of 2mm. As the length I of the y-cooling region is further reduced, the thermal lens becomes highly negative, e.g. with a refractive power of -3m'1 with a length of the y-cooling range of 1mm.
    In the diagram of FIG. 8, values of a calculation are also entered as stars, which well reflect the measured values obtained.
    The formation of a negative thermal lens with small expansions of the y-cooling region can be explained by the formation of a central depression in the temperature profile over the y-pumping region.
    By a suitable choice of the size of the y-cooling region can thus be achieved with respect to the y-direction disappearing or almost disappearing thermal lens. The length of the y-cooling region is chosen to be less than 70% and greater than 50% of the length L of the y-pumping region.
    The y-pumping region extends in both directions of the y-axis beyond the y-cooling region, preferably equidistant, i. the y-cooling area is located centrally in the y-pumping area with respect to the y-direction.
    Conversely, the length of the z-cooling region 27 of the laser medium 1 is advantageously greater than the length of the z-pumping region 29 of the laser medium 1. The extent of the z-cooling region in both directions of the z-axis beyond the z-pumping region will be so great chosen that inhomogeneities of
    Temperature distribution in the pumped volume of the laser medium 1 to the ends of its extension in the direction of the z axis are kept as small as possible.
    The beam profile of the forming laser mode is advantageously at least largely adapted to the profile of the excitation by means of the pump radiation 5 with respect to the y-direction, in particular by using a suitable gradient mirror. The beam profile of the laser beam 4 with respect to the y direction should thus have an intensity distribution which is shifted clearly in the direction of a rectangular profile relative to a Gaussian profile.
    Analogous to the pump radiation 5, a y-half-value range and a y-1 / e2 range of the laser beam 4 in the laser medium 1 and when leaving the laser medium 1 can be defined. The y-1 / e2 region of the laser beam thus represents a section of the y-axis, over which the intensity of the laser beam 4 has a value which is more than the maximum intensity of the laser beam 4 divided by e2. The y-half-value region of the laser beam 4 designates a section of the y-axis, over which the intensity of the laser beam 4 has a value which is more than half the maximum intensity of the laser beam 4.
    In particular, the laser beam 4 is formed such that the difference between the length of the y-1 / e2 region of the laser beam and the length of the y-half-value region of the laser beam is less than half the difference between the length of the y axis. 1 / e2 region and the length of the y-half-value region of an imaginary ray of the same wavelength having a Gaussian profile and whose length of the y-half-value region is equal to the length of the y-half-value region of the laser beam 4 and whose radiant energy is equal to Radiation energy of the laser beam 4 is.
    By the invention, for example, one, in particular pulsed, Nd: YAG laser with an average power of> 2 W and a beam divergence of <250 prad (half-angle divergence) in both transverse directions and one ΜΛ2 of <5, or also <3 Be prepared, without having to be installed in the external laser beam 4a or in the resonator symmetry and astigmatism compensating optics.
    Key to the reference numbers: 1 amplifying laser medium 26 y cooling area 2 inlet area 27 z cooling area 3 exit area 28 y pumping area 4,4a laser beam 35 29 z pumping area 5 pumping radiation 31 y half-value area 6 first side area 32 y half-power range 7 end mirror 33 y-1 / e2 region 8 outcoupling mirror 34 y-1 / e2 region 9 reverse prism 40 35 distribution 10 polarizer 36 distribution 11 Pockels cell 37 base surface 12 Lamda-Vietel plate 38 top surface 13 radiation source 14 optic 14a entrance surface 14b Cylindrical surface 14c Side surface 14d Exit surface 15 Bar 16 Laser diode 17 Laser beam 18 Carrier 20 Carrier 21 Heat sink 22 Heat sink 23 Second side surface 24 Cooling strip 25 Air gap
    权利要求:
    Claims (10)
    [1]
    1. Solid-state laser with a reinforcing laser medium (1) for generating a laser beam (4) and at least one laser diode (16) having pumping means (13, 14) from which a pump radiation (5) is generated, which on a first side surface ( 6) of the laser medium (1) which is parallel to a z axis and parallel to a y axis perpendicular to the z axis, in a direction perpendicular to the z axis and perpendicular to the y axis. A laser beam (4) runs parallel to the z-axis through the laser medium (1), the laser medium (1) lying on a plane parallel to the z-axis and parallel to the y-axis and the first side surface (6). opposite second side surface (23) is cooled by a heat sink (22), with which it is in thermal communication, wherein the length of a y-cooling region (26) smaller than the length of the second side surface (23) of the laser medium (1) in the direction d ery axis, wherein the y-cooling region (26) of the laser medium (1) denotes a section of the y-axis, over which a cooling strip (24) extends, over which the laser medium (1) on the second side surface (23) is thermally connected to the heat sink (22), wherein the length of a y-1 / e2 region (33) of the pump radiation (5) is smaller than the length of the first side surface (6) of the laser medium (1) in the direction of the y-axis and the first side surface (6) of the laser medium (1) extends beyond the y-1 / e2 region (33) of the pump radiation (5) in both y-axis directions, the y-1 / e2 region (33) of the pump radiation (5) denotes a section of the y-axis, via which the intensity of the pump radiation (5) on the first side surface (6) of the laser medium (1) has a value which is more than the maximum intensity of the pump radiation ( 5) on the first side surface (6) of the laser medium (1) divided by e2, characterized in that the longitudinal e of the y-cooling region (26) of the laser medium (1) is less than 70% and greater than 50% of the length of a y-pumping region (28) of the laser medium (1) and the y-pumping region (28) is in both directions Extends beyond the y-cooling region (26), wherein the y-pumping region (28) denotes a portion of the y-axis, over which 80% of the total absorbed by the laser medium (1) power of the pump radiation (5) is absorbed and at the two ends of the intensity of the pump radiation (5) is equal.
    [2]
    2. Solid state laser according to claim 1, characterized in that the difference between the length of the y-1 / e2 region (33) of the pump radiation (5) and the length of a y-half-value region (31) of the pump radiation (5) less is half the difference between the length of a y-1 / e2 region (34) and the length of a y-half-wave region (32) of an imaginary equal wavelength beam having a Gaussian profile and of which the length is one y half-power range (32) is equal to the length of the y-half-value region (31) of the pump radiation (5) and its radiant energy is equal to the radiant energy of the pump radiation (5), wherein the y half-value region (31) of the pump radiation (5) designates a portion of the y-axis, via which the intensity of the pump radiation (5) on the first side surface (6) of the laser medium (1) has a value which is more than half the maximum intensity of the pump radiation (5) the first side surface of the laser medium (1) is d the y-1 / e2 region (34) of the imaginary ray denotes a portion of the y-axis over which the intensity of the imaginary ray at the first side surface (6) of the laser medium (1) has a value greater than the maximum intensity of the imaginary ray on the first side surface (6) of the laser medium (1) divided by e2 and the y half-value region (32) of the imaginary ray designates a section of the y axis over which the intensity of the imaginary ray at the first Side surface (6) of the laser medium (1) has a value which is more than half of the maximum intensity of the imaginary beam on the first side surface (6) of the laser medium (1).
    [3]
    3. Solid-state laser according to claim 1 or 2, characterized in that a z-cooling region (27) of the laser medium (1) is greater than a z-pumping region (29) of the laser medium (1), wherein the z-cooling region (27) of Laser medium (1) denotes a portion of the z-axis, over which the cooling strip (24) extends, via which the laser medium (1) on the second side surface (23) with the heat sink (22) is thermally connected, wherein the z-pumping area (29) denotes a portion of the z-axis, over which 80% of the total of the laser medium (1) absorbed power of the pump radiation (5) is absorbed and at both ends of the intensity of the pump radiation (5) is equal.
    [4]
    4. Solid state laser according to one of claims 1 to 3, characterized in that the cooling strip (24) has a thermal conductivity of more than 5 W / mK.
    [5]
    5. Solid state laser according to one of claims 1 to 4, characterized in that apart from the region over which the cooling strip (24) extends, an air gap (25) between the second side surface (23) of the laser medium (1) and the heat sink (22) is located.
    [6]
    6. Solid-state laser according to one of claims 1 to 5, characterized in that the laser medium (1) has a prismatic shape, wherein the edges which bound the extension of the first side surface (6) of the laser medium (1) in the direction of the y-axis on both sides and the edges that bound the extent of the second side surface (23) of the laser medium (1) in the direction of the y-axis on both sides are parallel to the z-axis.
    [7]
    7. Solid state laser according to one of claims 1 to 6, characterized in that the laser medium (1) is arranged in a resonator.
    [8]
    8. Solid-state laser according to one of claims 1 to 7, characterized in that the laser beam (4) passes through the laser medium (1) running zig-zag and in this case lies in a plane which is at right angles zury axis.
    [9]
    9. Solid-state laser according to one of claims 1 to 8, characterized in that the laser beam (4) in the laser medium (1) and / or at its exit from the laser medium (1) has a beam profile in which the difference between the length of a y -1 / e2 region of the laser beam (4) and the length of a y half-value region of the laser beam (4) is less than half the difference between the length of a y-1 / e2 region and the length of ay Half wavelength range of an imaginary beam of the same wavelength having a Gaussian profile and of which the length of a y half-value range is equal to the length of the y half-power range of the laser beam (4) and its radiant energy is equal to the radiant energy of the laser beam (4) wherein the y-1 / e2 region of the laser beam (4) denotes a portion of the y-axis over which the intensity of the laser beam (4) has a value greater than the maximum intensity of the laser beam (4) divided by e2 beträ gt, wherein the y-half-value range of the laser beam (4) denotes a section of the y-axis, over which the intensity of the laser beam (4) has a value which is more than half the maximum intensity of the laser beam (4), wherein the y-1 / e2 region of the imaginary ray denotes a portion of the y-axis over which the intensity of the imaginary ray has a value greater than the maximum intensity of the imaginary ray divided by e2, the y-half-value Portion of the imaginary beam denotes a portion of the y-axis over which the intensity of the imaginary beam has a value which is more than half of the maximum intensity of the imaginary beam.
    [10]
    10. Solid state laser according to one of claims 1 to 9, characterized in that the amount of refractive power of a laser medium (1) formed in the operation of the solid-state laser thermal lens based on the y-axis is less than 0.5m * 1.
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    同族专利:
    公开号 | 公开日
    AT515674B1|2015-11-15|
    EP3117494A1|2017-01-18|
    WO2015135011A1|2015-09-17|
    US20170117681A1|2017-04-27|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    US20110064112A1|2009-09-11|2011-03-17|Zecotek Laser Systems, Inc.|Solid-state laser with waveguide pump path |
    WO2014019003A1|2012-08-03|2014-02-06|Daniel Kopf|Pump device for pumping an amplifying laser medium|
    JP4427280B2|2002-07-10|2010-03-03|新日本製鐵株式会社|Semiconductor laser device and solid-state laser device using the same|
    WO2004100331A1|2003-05-09|2004-11-18|Hamamatsu Photonics K.K.|Semiconductor laser device|US10794667B2|2017-01-04|2020-10-06|Rolls-Royce Corporation|Optical thermal profile|
    US10862261B2|2017-02-08|2020-12-08|Hamamatsu Photonics K.K.|Laser medium unit and laser device|
    AT521943A1|2018-12-14|2020-06-15|Dr Daniel Kopf|Q-switched solid-state laser|
    AT521942A1|2018-12-14|2020-06-15|Dr Daniel Kopf|Q-switched solid-state laser|
    AT522108A1|2019-01-31|2020-08-15|Montfort Laser Gmbh|Passively Q-switched solid-state laser|
    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    ATA184/2014A|AT515674B1|2014-03-14|2014-03-14|Solid-state lasers|ATA184/2014A| AT515674B1|2014-03-14|2014-03-14|Solid-state lasers|
    US15/126,017| US20170117681A1|2014-03-14|2015-03-10|Solid-state laser|
    PCT/AT2015/000038| WO2015135011A1|2014-03-14|2015-03-10|Solid-state laser|
    EP15716389.0A| EP3117494A1|2014-03-14|2015-03-10|Solid-state laser|
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