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    公开号:AT510116A1
    申请号:T0103110
    申请日:2010-06-22
    公开日:2012-01-15
    发明作者:Daniel Dr Kopf
    申请人:High Q Technologies Gmbh；
    IPC主号:
    专利说明:

    Patent Attorneys HefelScHofmann 23291/33 / ss 100604
    patent attorneys
    European Patent Attorneys
    European Trademark Attorneys
    Dl Herbert Hefel (until 2006)
    Dr. Ralf Hofmann Thomas Fechner 6806 Feldkirch, Austria Egelseestr 65a, PO Box 61 1
    The invention relates to a laser with a laser medium, which is excited in a pump region, and a standing-Welien-resonator having optical elements, of which a beam axis having, the laser medium passing laser beam is guided and a first and a second end mirror, the resonator comprising a first resonator section including the first end mirror and optionally further of the optical elements cooperating with the laser beam between the first end mirror and the laser medium, and a second resonator section including the second end mirror and others the optical elements which cooperate with the laser beam between the laser medium and the second end mirror, wherein at least one of the optical elements of the first resonator portion has a focusing formation, through which the beam axes of the laser beam, which at respective tiltings of at least one the optical elements arranged in the second resonator section have at least one crossing point, and wherein this crossing point or one of these crossing points of the beam axes of the laser beam lies in the pumping area of the laser medium or has a distance from the pumping area which is less than the Rayleigh length that corresponds to a section of the laser beam which lies between the laser medium and the nearest focusing optical element of the first resonator section.
    In general, lasers require resonators (also referred to as cavities) in which the laser beams pass through the laser medium (= active medium). In addition to standing-wave resonators (also referred to as linear resonators), in which the laser light between two end mirrors reciprocates, ring resonators are known in which the laser light is guided circumferentially, with basically two different directions of rotation are possible
    Mode-coupled femtosecond or picosecond lasers are generally provided with a
    Bank details T -r43 (0) 5522 73 137 Österreichische Postsparkasse Sparkasse der Stadt Feldkirch F +43 (0) 5522 73 359
    Account No. 92.111.622, 3LZ 60000 Account No. 0400-006300, bank code 20604 M office@vpat.at
    Swift Code: OPSKATWW Swift Code: SPFKAT2B) www.vpat.at IBAN AT55 6000 0000 9211 1622 IBAN: AT70 2060 4004 0000 6300 VAT ATU 65652215 the folded resonator {= "extended cavity"), especially if the pulse repetition frequency is in MHz Area should lie. In order to enable a compact construction at such a repetition frequency, a plurality of folding mirrors or deflecting mirrors are used. The laser beam strikes the main plane of the folding mirror at an incident angle close to 0 ° (+/- 10 °) to the surface normal. Such folding mirrors may be flat or have a curvature, so that they are formed as a concave mirror. For example, a femtosecond laser at 20 MHz has a resonator length of 7.5 m. The number of reflections required on folding mirrors then results from the length of the laser housing. For example, laser cases 56cm in length are commercially available. Frequently used pulse repetition frequencies are in the range of 20-120MHz.
    A problem with such resonators is the sensitivity to tilting of optical elements of the resonator. Commercially available resonators have a sensitivity to tilting of the optical elements in some optical elements such that a tilting of the optical element with respect to the adjusted (^ optimal) state by an angle of 50prad results in a power penalty of several percent due to shifts the beam axis of the laser mode opposite the pumping area of the laser medium. Usually, the optical elements of a laser resonator are mounted on a common support member, which is formed by a plate, a monolithic block or a mechanically stable linkage. The mirror elements of the resonator, which consist of the actual reflective mirror coating and the substrate (usually made of glass) on which the mirror coating is applied, are held in-usually metallic mirror holders, which in turn are fastened to the carrier part. This results in the problem that different materials meet: glass (as a mirror substrate) on the one hand and metals such as aluminum and stainless steel on the other hand. The thermal expansion is significantly different, so that changes in temperature either a voltage and / or a shift results against each other.
    An angular stability of better than 50 prad is technically difficult or only very difficult to achieve when assembling materials with different coefficients of expansion (taking into account environmental influences and over a period of several years): it means that a mirror surface with an extension of 10 mm at If one considers that several mirror elements can add up their tolerances, then the stability requirement for the individual mirror must be significantly increased. The surface roughness of milled or drilled metallic surfaces is usually 0.4 to 0.8 pm and thus can not provide the desired support accuracy usually.
    Pulsed laser beams can also be generated in a manner other than mode-locking, in particular by Q-switching. Typical pulse durations are in the nanosecond range.
    A mode-locked femtosecond solid-state laser is described, for example, in F. Brunner et al., "Diode-pumped femtosecond YbiKGdfWO ^ laser with 1.1 -W average power", OPTICS LETTERS, 2000, Vol. 25 (15), 1119-1121 , The folded standing wave resonator is here in the form of a so-called "delta cavity". educated. The laser medium formed by Yb: KGW is arranged in the laser beam in the region between two concave mirrors of the resonator, each having a radius of curvature of 200 mm. The beam radius (or mode radius) is here at the location of the laser medium less than one-tenth of the beam radius at the concave mirrors, the mirrors of this resonator have relative to tilting relatively high sensitivities at the location of the laser medium.
    Delta configurations of resonators are known in many other embodiments. Other known embodiments of resonators are, for example, so-called Z configurations.
    Further developments of pulsed lasers, in particular mode-locked lasers, are evident, for example, from EP 1 692 749 B1, EP 1 588 461 B1 and EP 1 687 876 B1 and the publications cited therein. Considerations for measures to reduce adjustment sensitivities of optical elements of a resonator are already included in the aforementioned EP 1 588 461 B1, for example. Here, an adjustment element is used to compensate for adjustment errors, wherein a back reflection of the laser beam takes place in itself or slightly offset, in particular by a curved mirror, or the laser beam collimated is guided on a resonator, in particular by a reflective or refractive element. Reflections on the orientation sensitivity of optical
    For example, resonators can also be found in the "Encyclopedia of Laser Physics and Technology". www.rp-photonics.com/aliqnment sensitivitv.html. This encyclopedia has also appeared in book form "Encyclopedia of Laser Physics and Technology", Paschotta, Rüdiger, 2008, ISBN-10: 3-527-40828-2 (Wiley-VCH, Berlin).
    From the earlier priority, not prepublished European patent application with the application number EP 09107189.1, the integral formation or the rigid connection of two optical elements of the resonator is apparent to the tilt sensitivity to these optical elements with respect to the position of the beam axis or its inclination at a other of the optical elements of the resonator. The same direction tilting of these two coupled optical elements in this case has opposite effects on the position of the beam axis or its angle in the other of the optical elements.
    The object of the invention is to provide a laser of the type mentioned, in which with respect to the Kippempfindlichkeit at least one of the optical elements of the resonator, an improvement is achieved. According to the invention, this is achieved by a laser having the features of claim 1.
    In the laser of the invention, at least one of the optical elements of the first resonator section has a focusing configuration. If only the first end mirror is arranged as optical elements in the first resonator section, it is therefore designed as a concave mirror. If, in addition to the first end mirror, at least one further optical element is arranged in the first resonator section, then the first end mirror and / or at least one of the further optical elements arranged in the first resonator section is focused. Such training is common. In such an embodiment, if, starting from an adjusted state, at least one of the optical elements of the second resonator section is tilted with respect to its adjusted position, the steel layer of the laser mode is changed, i. the beam axis (= optical axis) of the laser beam in the resonator. The beam axes occurring with different tilting of one of the optical elements of the second resonator section and / or with tilting of different optical elements of the second resonator section intersect here in a common crossing point lying between two optical elements of the resonator or in two or more crossing points which each lie between two optical elements of the resonator. The laser medium is arranged so that this crossing point or, in the
    Fall of more than one crossing point, one of these crossing points in the pumping area of the laser medium or close to this lies. In any case, the distance of the crossing point from the pumping region is smaller than the Rayleigh length, which belongs to the section of the laser beam which lies between the laser medium and the nearest focusing optical element of the first resonator section (which may possibly be the only focusing optical element of the first resonator section).
    Due to this arrangement of the laser medium, tilting of optical elements in the second resonator section results in no displacement at the location of the pumping area of the laser medium (if the crossing point lies in the pumping area) or only a slight shift (if the crossing point has a small distance from the pumping area). the beam axis with respect to the pumping area, but only to an angular change of the beam axis. Thus, the sensitivity of the laser has been reduced to virtually zero in terms of power over tilts of the optical elements located in the second resonator section. Only the optical elements of the first resonator section are sensitive to adjustment in this sense, wherein the first resonator section, for example, can have only the first end mirror as the only optical element.
    Instead of tilting or in addition to this, a misalignment of an optical element may also have a transverse displacement relative to its adjusted position. These can occur, for example, due to (thermal) tensions. In the case of flat mirrors, the beam position does not change as a result, however, in the case of curved mirrors or in the case of lenses in which such a lateral displacement can be represented as an optionally additional contribution to the tilt, which depends on the radius of curvature. For a misalignment in the sense of a lateral shift applies to curved mirrors and lenses thus analogous as previously performed in connection with the tilting. Again, there is a change in the beam axis, wherein the different beam axes intersect in at least one crossing point, in the same or the same as in a pure tilting.
    The beam axis, which forms in the adjusted state of the optical elements, ie without misalignment and thus the "ideal". optical axis of the laser beam or laser mode is hereinafter referred to as the center axis of the laser beam. This center axis preferably intersects the main plane of the respective optical element at the intersection of the main plane of this optical element with the axis of symmetry of this optical element.
    As tilting of the optical elements in order to determine the at least one crossing point, such tilting is preferably considered, which take place starting from the adjusted position of the respective optical element about a respective tilt axis, which is perpendicular to the axis of symmetry of the optical element and through the intersection of the main plane of the optical element runs with its axis of symmetry. The angular range of the tilting lies in any case within the limits in which the laser mode is still formed. Furthermore, the tilting range is within the limits within which the laser beam with its entire beam diameter is still within the optical surfaces of the optical elements. The optical surfaces are the surfaces of the optical elements interacting with the laser beam. These may be reflecting surfaces (of mirrors) as well as passage surfaces (lenses, if any) and a combination thereof (e.g., a coupling-out mirror).
    In practice, when tilts occur about axes other than the aforementioned tilting axis, they may be considered as superimposing a tilt about said tilting axis with a transverse displacement and a displacement in the direction of the central axis. Shifts in the direction of the central axis can generally remain approximately unnoticed.
    The laser medium is also an optical element with optical surfaces, which influences the laser beam. Thus, a thermal lens is formed by the laser medium (as optical elements of the resonator, however, only the optical elements present in addition to the laser medium which guide the laser beam are considered in this document).
    If there is more than one crossing point of the laser beams, the pumping area of the laser medium is preferably placed at or near the point of intersection closest to the first end mirror. It can thereby minimize the number of the adjustment-sensitive optical elements.
    According to the invention, the radius of the laser beam (= radius of the laser mode) is at least over the portion of the laser beam which is between the laser medium and the nearest one. *** " · * · · * Ι · t ··· * * «f * f I« '4 · * «« «*** *****» * • * ^ I * + ·· # * * · focus optical element of the first resonator section is less than five times, preferably less than three times, more preferably less than twice, the radius of the laser beam in the pumping region of the laser medium. Thus, relatively small changes in the beam radius or relatively small divergences or convergences of the laser beam are present at least over this section of the laser beam. As a result, in the embodiment according to the invention, the tilt sensitivity of at least one optical element of the first resonator section, in particular of the focusing element of the first resonator section or one of the focusing elements of the first resonator section (preferably at least that of the laser medium) and / or at least one additionally existing folding mirror of the first resonator section can be reduced. In advantageous embodiments of the invention, the radius of the laser beam in the entire first resonator section is less than five times, preferably less than three times, more preferably less than twice the radius of the laser beam in the pumping region of the laser medium.
    For example, for a tilt of 100prad, the power-related tilt sensitivity for all optical elements of the first resonator section may be less than 5% (the percentage tilt / turn sensitivity is discussed below). In the embodiment according to the invention, the distance of the pumping region of the laser medium from the focusing optical element of the first resonator section or, in the case of a plurality of focusing optical elements in the first resonator section, from the nearest focusing optical element of the first resonator section is advantageously less than three times the Rayleigh length. which belongs to the portion of the laser beam (with respect to its actually formed or interpolated beam waist) which lies between the laser medium and the nearest focusing optical element of the first resonator section. The interpolated beam waist is to be used here, for example, when the laser beam already impinges on the laser medium before reaching the beam waist (the focus being changed by the thermal lens formed by the laser medium). The distance of the pumping region of the laser medium from the nearest focusing optical element is, of course, determined in the unfolded state of the resonator, if there is a plane folding mirror between the laser medium and this focusing optical element.
    The unfolded state of the resonator results in a known manner from the fact that the z-axis of the resonator, along which the beam axis of the laser beam runs in the adjusted state of the optical elements, is shown in a straight line.
    The radius of the laser beam or laser mode is the distance from the beam axis at which the intensity of the laser beam drops to a value of 1 / e 2 (about 13.5%). The diameter of the laser beam is twice the value of the radius of the laser beam.
    The length of the pumping region of the laser medium, with respect to the direction of the central axis of the laser beam, preferably with respect to all the beam axes with tilting of optical elements, is advantageously shorter than half the value of the Rayleigh length, particularly preferably less than a fifth. the value of the Rayleigh length, Conveniently, the crossing point, which is in or near the pumping range of the laser medium, is located between the first and the second resonator section,
    The focal length of the focusing optical element of the first resonator section or, in the case of several focusing optical elements in the first resonator section, of the focusing medium closest to the laser medium in the first resonator section is less than 100 mm, preferably less than 50 mm, in an advantageous embodiment of the invention. Depending on the embodiment, this focal length can also be less than 20mm or less than 10mm, with values of less than 5mm are possible. It is thus conveniently used relatively strong focusing optical elements, of which the laser medium has a relatively small distance.
    As already mentioned, the resonator of a laser according to the invention is in particular folded, that is to say as a so-called "extended cavity". In this case, in addition to the first and second end mirrors, there is at least one fold deflecting the laser beam, in particular by more than 160 °, folding mirrors (deflecting mirrors). The laser beam thus impinges on the latter at an angle of incidence from 0 ° to 10 ° to the surface normal to the main plane of the folding mirror. Preferably, a plurality of such folding mirrors are present, for example four or more. In advantageous embodiments, more than ten such folding mirrors may also be present. »4 *» ** · * »··· * * ·« * * r *
    Depending on the embodiment, the deployed length of the resonator is more than 1 m, in particular more than 5 m, and in other embodiments shorter resonator lengths may also be present.
    In an advantageous embodiment of the invention, the length of the first resonator section is less than 200 mm, preferably less than 100 mm. In further advantageous embodiments, this length is less than 40 mm, preferably less than 20 mm.
    Preferably, the length of the first resonator section is less than one fifth of the length of the second resonator section, particularly preferably less than one tenth of the length of the second resonator section. In further advantageous embodiments, the length of the first resonator section is less than one fiftieth of the length of the second resonator section.
    When talking about the length of a resonator section, this refers to the length in the deployed state.
    In an advantageous embodiment of the invention, the laser is ausgebrl-det as a pulse laser. For example, a mode coupling may be provided, wherein the pulse duration may be in particular in the femtosecond or picosecond range. In other embodiments, Q-circuits may be provided, wherein the pulse duration may be in particular in the nanosecond range.
    When formed as a pulse laser, the local length of the pulse is desirably smaller than the unfolded resonator length, preferably less than one tenth of the unfolded resonator length. Values of less than 150 MHz are favorable for the pulse repetition rate in many embodiments, the unfolded length of the resonator correspondingly being greater than 1 m. Advantageous embodiments provide pulse repetition rates of less than 50 MHz, ie resonator lengths of more than 3 m. For designs of pulse repetition rates of less than 30 MHz, the resonator length is correspondingly greater than 5 m. Especially with long resonators with many folding mirrors reduced tilting sensitivities are of particular importance.
    To calculate the displacement and angular deviation of the beam axis of the laser beam (r, r ') with a tilt of an optical element relative to the central axis or ideal axis {without tilting), the calculation method can be used, as for example by Siegman Anthony E .: "Lasers", University Science Books 1986, pages 607-614. There, an extension of the known ABCD matrix calculation method for calculating laser cavities on the so-called ABCDEF calculation method is described. Through these, the tilt sensitivity of resonators can be determined by means of the matrix element "F". be calculated. For this purpose, an additional fictitious tilting element is inserted in the resonator at the location of a considered optical element for which the tilt sensitivity is to be determined. If the considered optical element is a folding mirror and the effect of a tilting of the folding mirror is to be determined by 100 prad, then the tilting element has a 3x3 matrix with following values ABCDEF (100prad) = {A, B, E; C, D, F; 0, 0, 1} = {1,0, 0; 0, 1, 2e-4; 0, 0, 1). It is considered here that tilting of the folding mirror by 100 prad results in a tilting of the optical axis by 200 prad, so that in the matrix of the tilting element the angular tilting value F is assigned a value of 2e-4. Considering the tilt of a lens by 100 prad, the tilt value would be F = 1e-4.
    To calculate the initial coordinates for the optical axis of the laser beam at the first end mirror with a tilting element ABCDEF {100 prad) inserted at point Z in the resonator, an eigenvector calculation is performed. The initial coordinates (r0, r'0) are calculated in which these initial coordinates of the beam axis in a resonator cycle are again "in themselves". be imaged. For the calculation, the vector (r, rr, 1) is used, where r represents the transverse displacement of the laser axis and r 'represents its inclination with respect to the central axis. If there are no tilts of optical elements, so all elements F are 0, then (r0, r'0) = (0, 0).
    From the requirement of mapping the initial coordinates of the optical axis to a resonator cycle "in itself " It follows that all beam axes of the laser beam forming at different inclinations must be perpendicular to the optical surface of the first end mirror (this also applies to the second end mirror).
    Propagation of the beam axis by the resonator, starting from the initial coordinates, is calculated by dividing each individual optical element, i. It is thereby multiplied by the vector (r, r ', 1) for each optical element at a given location z in the resonator, the deviation r, r' of the beam axis from the central axis (ie without tilting of an optical element). Thus, the course of " eigenaxis " (r, r ') for a given tilt of one of the optical elements over the entire resonator.
    From the deviation (rmeG, r ^ ') of the beam axis of the laser beam at the location of the laser medium, when one of the optical elements is tilted, for example by 100 prad, the effect of this tilt on the power of the laser can be determined. In particular, the value rmed indicates the shift of the beam axis in the laser medium with respect to the adjusted or optimal state (this adjusted state would be given by rmed = 0). The ratio of the displacement of the beam axis relative to the beam radius (mode radius) wmed in the laser medium, to which the radius of the pumping area is tuned, can be used as a quantitative measure of the tilt sensitivity or adjustment sensitivity of the laser resonator for the tilting of the observed optical element by 100 prad The adjustment sensitivity is given in%, values of 10% and above usually result in a noticeable tilting sensitivity, values significantly above this an undesirably high tilting sensitivity.
    The calculation is based on the paraxial approximation. The beam path within the laser resonator is at least partially, preferably completely, designed as a free-beam optic, that is not guided between the optical elements in a waveguide (from a medium other than air).
    Previously, only the tilt of one of the optical elements was considered. The value E in the ABCDEF matrix for the misalignment of an optical element in the sense of a transversal shift was set to 0. The calculation can analogously be used for the transverse displacement of a considered optical element, the "E " a corresponding value is assigned. For optical elements with curved surfaces (curved mirrors and lenses), an approximately (additional) tilting of the optical element can instead be applied.
    The beam position parameters of the coupled-out output beam of the laser may be of interest, since a laser is usually integrated in an optical application system, the tolerances for the incoming laser beam in position (position and angle at * * * * * «* t * *« * * · 12 * ** ** * ·· · a defined position). In addition to the effect of the tilting (and / or transverse displacement) of an optical element on the power of the laser is thus also of interest to what extent in a tilting (and / or transverse displacement) of an optical element to a transverse displacement and / or angular deviation of the Beam axis comes at the coupling element of the laser. This can be calculated with the same method, namely by propagating the initial value of the beam axis (r0, r'0) through the resonator using the ABCDEF matrix calculation up to the output coupler (unless the output coupler corresponds to the beginning of the resonator anyway ).
    In order to reduce the sensitivity of the transverse displacement and / or angular deviation of the beam axis at the output coupler, it is preferred that at least two optical elements of the resonator, the opposite in a same direction tilting effects on the transverse displacement and / or angular deviation of the beam axis Auskoppler have, wherein these two optical elements z are located at different locations in the resonator, integral with one another or rigidly connect to each other and to mount together on a support member of the resonator. In particular, these two optical elements can be two folding mirrors. Between these two integrally formed with each other or rigidly connected together and mounted folding mirrors is thus at least one other folding mirror.
    In the case of integral formation, the optical surfaces of the two optical elements are located on a common base body. In the case of the rigid connection of the two optical elements, the optical surfaces of the two optical elements are at different, rigidly interconnected bodies, which are mounted on a common support on a support member of the resonator, wherein they are preferably adjustable together. At least a part of the further optical elements of the resonator are also mounted on the carrier part, specifically via separate holders.
    If the two integrally formed or rigidly interconnected optical elements in a same direction tilting have opposite effects on the displacement and / or angular deviation in another of the optical elements of the resonator, so by such a one-piece design or rigid connection of two optical elements the at a tilt of these optical elements resulting displacement and / or angular deviation of the
    Beam axis can be reduced at this other optical element. For example, a reduction in the change in the slope of the output beam may be important. Thus, the displacement and / or the angular deviation of the beam axis is reduced in an optical element of the laser, which is sensitive to such a displacement and / or angular deviation. For example, this optical element, which is sensitive to displacement in particular, could be an acousto-optic or electro-optic modulator.
    In an advantageous embodiment of the invention, the optical surfaces of the two integrally formed or rigidly interconnected optical elements are curved and have different centers of curvature and / or radii of curvature or even and lie in mutually perpendicular planes or is the optical surface of one of these two optical elements curved and the optical surface of the other of these two optical elements even.
    Further advantages and details of the invention are explained below with reference to the accompanying drawings. In this show:
    Fig. 1 is a schematic representation of a laser arrangement according to the prior art; 2 shows a representation of the beam radius (mode radius) and the optical elements of the resonator, in the deployed state, according to a second embodiment according to the prior art;
    Fig. 3 is a schematic diagram of a laser arrangement according to a possible embodiment of the invention;
    4 shows a schematic representation of a specific laser arrangement according to a first exemplary embodiment of the invention;
    FIG. 5 shows the illustration of the beam radius for the embodiment of FIG. 4 in the unfolded state of the resonator; FIG.
    6 and 7 representations analogous to Figures 4 and 5 for a second concrete embodiment of the invention.
    Fig. 8 is a schematic diagram of another possible embodiment of the invention; 9 and 10 representations analogous to Figures 4 and 5 for a third concrete embodiment of the invention.
    11 shows an enlarged detail of FIG. 10;
    FIGS. 12 and 13 show schematic embodiments of two coupled optical elements of the resonator. • * * · · Ά · ·· 1 $ ·
    A prior art laser device according to the previously mentioned article F. Brunner et al., "Diode-pumped femtosecond Yb: KGd (W04) 2 laser with 1.1 -W average power", OPTICS LEITERS, 2000, Vol. 25 (15 ), 1119-1121 is shown schematically in FIG. In a standing-wave resonator, a laser medium 4 is arranged in the form of Yb: KGW. The laser arrangement comprises a resonator with a first end mirror 1, which is designed to perform a mode-locking function as a SESAM mirror. The resonator further comprises a second end mirror 2, which is formed here by a partially transparent training as an output coupler for the output beam 3 of the laser. Between the first end mirror 1 and the laser medium 4, folding mirrors 5, 6 in the form of spherical concave mirrors with radii of curvature of 200 mm are arranged as further optical elements. The folding mirror 6 is in this case designed as a dichroic mirror and through this pumping of the laser medium 4 takes place. This purpose, a laser diode 7, the beam is guided through optical elements 8, 9, 10 and through the folding mirror 6 into the laser medium 4. Between the second end mirror 2 and the laser medium 4, a folding mirror 11, prisms 12, 13 and a diaphragm 14 are arranged. By the folding mirror 11 takes place in an analogous manner as by the folding mirror 6, an optical pumping of the laser medium 4 by means of a second laser diode 7 and optical elements 8, 9, 10th
    In the further embodiment of the prior art shown in FIG. 2 on the basis of the beam diameter of the unfolded cavity and the associated optical elements shown schematically below, TirSaphir is used as the laser medium 15. The resonator, in which the laser medium 15 is arranged, comprises a plane first end mirror 16, which serves as an output coupler for the laser beam, a plane second end mirror 17, which is designed for mode coupling as a SESAM mirror, and between the first end mirror 16 and the Laser medium 15 arranged folding mirror 18,19, of which the folding mirror 18 is flat and the folding mirror 19 is a concave mirror with a radius of curvature of 300mm, and arranged between the laser medium 15 and the second end mirror 17 folding mirror 20, 21, 22, of which the folding mirror 20 is a concave mirror having a radius of curvature of 300mm, the folding mirror 21 is a plane mirror, and the folding mirror 22 is a concave mirror having a radius of curvature of 200mm. The distances of the optical elements 16-22 of the resonator and the position of the laser medium 15 in the resonator can be seen from Fig. 2, since their positions on the ordinate (= z-axis), the distance from the first end mirror 16 in the unfolded state of the resonator indicates) whose scale is given in mm are drawn. The distance between the laser medium 15 and the adjacent folding mirrors 19, 20 is 160 mm in each case. The laser medium 15 has a thickness of 1 mm. The abscissa indicates the radius of the laser beam in μιτι (above tangential, below sagittal). The radius of the laser beam over the course of the z-axis is shown.
    From Fig. 2 it is clear that the laser beam at the location of the laser medium has a pronounced constriction, which is accomplished by the use of the curved folding mirror 19, 20, whose radius of curvature is 300mm. In the case of the two concave mirrors 19, 20, the mode radius is more than ten times greater than in the case of the laser medium 15.
    Fig. 3 shows a schematic diagram of a first possible embodiment of the invention. The laser has the active laser medium 15. In particular, it is a solid-state laser. For example, the laser medium 23 may be Yb: KYW (with, for example, 5% Yb doping) or other ytterbium-doped tungstates, such as, for example, Yt. Yb: KGW act. The laser medium 23 is arranged in a standing wave resonator comprising a first end mirror 24 and a second end mirror 25. In this embodiment, the first end mirror 24 is the only focusing optical element of the first resonator section 26. However, other optical elements, for example one or more plane folding mirrors, could be arranged between the first end mirror 24 and the laser medium 23.
    The second resonator section 27 comprises, in addition to the second end mirror 25, further optical elements. These are symbolized here in their entirety by the ABCD matrix 28 of the overall system of these optical elements. These further optical elements of the second resonator section 27 may, for example, be formed by one or more folding mirrors or comprise such folding mirrors.
    The decoupling of the output beam 29 indicated by dashed lines in FIG. 3 can take place, for example, through the first end mirror 24. A decoupling by the second end mirror 25 or by another of the optical elements of the resonator is possible.
    The pumping of the laser medium 23 is not shown in FIG. For example, this could be done by the first end mirror 24, which is designed to be dichroic for this purpose (the decoupling would then take place at another optical element). Specific examples of pumping are described below. • ψ • ♦ «t« 16 *
    Preferably, it is a pulsed laser. The pulse repetition rate may be relatively low, for example less than 30 MHz, resulting in a correspondingly large overall length of the resonator and a corresponding number of folding mirrors, in order nevertheless to achieve a compact design, e.g. with four or more folding mirrors. In particular, the laser can be designed as a mode-locked laser. In order to achieve a mode coupling, a saturable absorber may be provided, for example one of the end mirrors or one of the folding mirrors as a saturable absorber mirror, such as SE-SAM mirrors. Other passive mode couplings, such as by the Kerr lens effect, or active mode couplings by acousto-optic modulators or electro-optic modulators, such as the Pockels cell, may also be provided.
    If short pulse durations are desired, in particular in the picosecond range or shorter, at least one of the mirrors of the resonator is formed with a negative group velocity dispersion.
    A pulsed laser, in particular with pulse durations in the nanosecond range, could instead be achieved by a Q-switching. Furthermore, the laser could also be operated continuously, ie as a continuous wave laser,
    If the optical elements of the resonator have their ideal positions (= "adjusted layers"), ie there is no misalignment in the form of a tilting and / or transverse displacement, the result for the beam axis 30 (= optical axis) of the laser beam or Lasermodes indicated in Fig. 3 as a solid line center axis. With a tilting of one or more of the optical elements in the second resonator section 27, deviations from this central axis occur. Some such deviating beam axes 30 'are indicated in Fig. 3 by dashed lines. At each point z (= distance from the first end mirror 24 or from its center plane relative to the unfolded state of the resonator), there is a distance (r) of the tilt axis resulting beam axis 30 'from the central axis 30 and an angle ( r ') against this. Since the beam axes of forming laser modes must be perpendicular to the optical surface of the first end mirror 24, the beam axes 30, 30 'intersect at a common intersection point 31. The laser medium 23 is arranged so that this intersection point 31 in the pumping region of Lasermediums 23 comes to rest, so here is arranged at a distance from the first end mirror 24, which is equal to the radius of curvature of the first end mirror 24. In the case of a transverse displacement of one of the optical elements, either the beam axis 30 remains unchanged (with a shift of a plane mirror) or this displacement leads to a different beam axis 30 ', which also leads through the crossing point 31. Thus, the sensitivity related to the laser power has been reduced to zero with a tilt and / or shift of those elements located in the second resonator section 27.
    Low sensitivity can also be achieved by arranging the pumping area of the laser medium 23 near the crossing point 31, the distance from the crossing point 31 being smaller than the Rayleigh length that belongs to the portion of the laser beam that exists between the laser medium 23 and the nearest focusing optical element of the first resonator section, this is here the first end mirror 24.
    A tilting or transverse displacement of one or more of the optical elements lying between the second end mirror 25 and the laser medium 23 can be represented by an ABCDEF matrix of the overall system of these optical elements.
    The system ABCD is chosen by a person skilled in the art according to the desired properties, e.g. Length of the resonator, number and position of folding mirrors for compacting, desired beam radius w in the laser medium, desired beam cross section at the second end mirror 25 (in particular if this example performs a mode-locking function such as a SESAM mirror), radius of curvature of the first end mirror, etc. For the second end mirror 25, instead of a plane mirror, a concave mirror can also be used. Usually, the size of the pumping region of the laser medium 23 is adapted to the beam diameter of the laser mode such that the respective beam diameters at the location of the laser medium are approximately equal. The optimum is determined in the experiment. With a beam diameter of the laser mode of 200 pm (i.e., radius w = 100 pm) in the laser medium 23, it may be a good idea to also design the pump beam diameter in the laser medium to about 200 pm. This can be achieved in the concrete structure, for example, by imaging the light of a commercially available, fiber-coupled pump laser diode with a core diameter of 200 μm and a numerical aperture of 0.22 with a simple 1: 1 imaging in the laser medium, e.g. with two Lin- * ··· »* * * 9 * t I» · · Μ * ** · ·
    Of the same focal length, of which the first assumes the function of the col- limation and the second the function of the re-focusing.
    The tilting, which lead to deviating from the central axis 30 beam axes 30 ', for example, at +/- 100 prad and / or +/- 200 prad and / or +/- 300 prad.
    In any case, the radius of the laser beam in the first resonator section 26 is less than five times the value of the radius of the laser beam in the pumping region of the laser medium, preferably less than three times.
    A concrete embodiment of a construction according to the schematic diagram of Fig. 3 is shown schematically in Fig. 4. The first end mirror 24 is formed by a concave mirror with a radius of curvature of 25mm. The distance of the laser medium 23 from the first end mirror 24 (based on the unfolded state) is equal to the radius of curvature of the first end mirror 24, in the present Ausführungsbeispiei so 25mm. Between the first end mirror 24 and the laser medium 23 is further a pleated, dichroic coated folding mirror 32, which represents the Pumpeninkoppelspiegel. The pumping takes place in the above described manner by means of a laser diode 33 and the two lenses 34, 35. The laser medium is for example of: KYW with e.g. 5% Yb doping formed. For example, the laser medium may have a thickness of 1 mm (measured in the z-direction),
    The first end mirror 24 and the folding mirror 32 together form the first resonator section.
    The second end mirror 25 is formed by a plane mirror, possibly by a SESAM mirror! for fashion coupling. Between the laser medium 23 and the second end mirror 25, folding mirrors 36-39 serve to fold the laser beam. The folding mirror 36 is arranged at a distance of 182 mm from the laser medium 32 and has a radius of curvature of 400 mm. The folding mirror 37 is arranged at a distance of 400 mm from the folding mirror 36 and has a radius of curvature of 400 mm. The folding mirror 38 is arranged at a distance of 400 mm from the folding mirror 37 and has a radius of curvature of 400 mm. The folding mirror 39 is arranged at a distance of 400 mm from the folding mirror 38 and has a radius of curvature of 800 mm. The second end mirror 25 is arranged at a distance of 400 mm from the folding mirror 39. • * * 19 *
    The total length of the resonator is 1809mm for the single span, 3618mm for the round. The round trip time is thus approx. 12 ms, which leads (with mode coupling) to a pulse repetition rate of 82.9 MHz.
    This resonator has a beam radius of about 100 pm at the location of the laser medium.
    The laser can be installed, for example, in a housing with a length of 450mm and a width of 71mm.
    The folding mirror 32 could be dispensed with and it could be pumped directly through the first end mirror 24 if it is coated with dichroic reflection, ie highly reflecting at 1040 nm and at the same time highly transmissive for the pump wavelength of 981 nm usual at Yb: KYW. The outcoupling of the output beam 22 could then take place, for example, at the second end mirror 25. The mode-locking could then be realized by one of the other optical elements.
    The folding mirrors 36, 38 and the folding mirrors 37, 39 are advantageously coupled together, as will be explained in more detail below.
    Fig. 5 shows an analogous to Fig. 2 representation of the radius of the laser beam in μιτι measured as a function of the distance from the first end mirror 24 (based on the unfolded state of the resonator), ie in the z-direction. The locations at which the optical elements and the laser medium are arranged are indicated by dashed lines and these are designated by the reference numerals of these elements. The first and second resonator sections 26, 27 are also indicated
    As can be seen from FIG. 5, the radius of the laser beam in this exemplary embodiment is smaller than the radius of the laser beam in the laser medium in the entire first resonator section.
    FIGS. 6 and 7 show analogous representations to FIGS. 4 and 5 for a second concrete exemplary embodiment. Analogous parts are provided with the same reference numerals.
    The first end mirror here has a radius of curvature of 6.5 mm and the distance of the laser medium 23 from the first end mirror is correspondingly 6.5 mm. The laser medium 23 corresponds to that of the first embodiment. The pumping of the laser medium takes place in the manner described above, here directly through the first end mirror 24. The folding mirror 36 has a radius of curvature of 100mm and is located at a distance of 48mm from the laser medium 23. The folding mirror 37 has a radius of curvature of 400mm and is located at a distance of 400mm from the folding mirror 36. The folding mirror 38 has a radius of curvature of 400mm and is located The folding mirror 39 has a radius of curvature of 800mm and is located at a distance of 400mm from the folding mirror 38. The second end mirror 25 is flat and located at a distance of 400mm from the folding mirror 39th
    The second end mirror 25 can serve as an output coupler for the (not shown here) output beam. A mode coupling could then be taken over by another optical element. On the other hand, the second end mirror 25 could also be formed as a mode coupler, wherein another optical element forms the output beam for the output beam.
    The beam radius in the laser medium here is about 35-40 mm.
    In a further specific embodiment, a larger beam radius in the laser medium, for example, of 170 μιτι could be achieved. For this purpose, the first end mirror 24 could have a radius of curvature of 75 mm and the laser medium 23 thus be arranged at a distance of 75 mm from the first end mirror. The folding mirror 36 could be arranged at a distance of 136 mm from the laser medium 23 and have a radius of curvature of 400 mm. The folding mirrors 37-39 and the second end mirror 25 could be designed in accordance with the first and second concrete embodiment and have the distances there from one another or from the folding mirror 36. Such a design would be suitable, for example, for the mode of operation of a regenerative amplifier in which higher energies and peak powers prevail, so that the optical damage threshold can be a problem.
    Fig. 8 shows a schematic diagram of another possible basic embodiment. It is used here as the first end mirror 24 'a plane mirror and between the first end mirror 24' and the laser medium 23 is a further optical element of the first resonator 26 is a focusing optical element, for example in the form of a concave mirror. The second resonator section 27 has as optical elements the second end mirror 25 and further, for this purpose a common ABCD
    Matrix 28 summarized optical elements. The beam axis 30, which represents the central axis without a misalignment of optical elements of the second resonator section 27, is again shown as a solid line. For the beam axes 30 'forming during a misalignment, again the condition applies that they are perpendicular to the optical surface of the first end mirror 24'. A crossing point 31 of the beam axes 30, 30 'is therefore present at the focus of the optical element 40 and the laser medium 23 or its pumping region is arranged there. Again, the laser medium 23 could also be spaced from the intersection 31, the distance being less than the Rayleigh length.
    A concrete embodiment of the basic embodiment shown in Fig. 8 is shown in Figs. 9 and 10. These are analogous to FIGS. 4 and 5 representations.
    At a distance (of, for example, 40 mm) from the plane first end mirror 24 'is the optical element 40 formed by a concave mirror with a radius of curvature of 150 mm. At a distance of 75 mm thereof, ie half the radius of curvature, is the laser medium 23. This corresponds to that of the first embodiment. The pumping can be done through the optical element 40 in the manner already described, wherein this optical element 40 is formed as a dichroic mirror. At a distance of 100mm from the laser medium is the folding mirror 3ό, which has a radius of curvature of 400mm. The folding mirrors 37-39 and the second end mirror 25 and their distances from each other and the folding mirror 36 are the same as described in the first embodiment.
    The mode radius in the laser medium here is 183 pm.
    Between the first end mirror 24 'and the optical element 40 and / or between the optical element 40 and the laser medium 4, a folding mirror could be arranged.
    FIG. 11 shows an enlarged view of a section of FIG. 10. It can be seen particularly clearly that the laser beam runs between the laser medium 23 and the adjacent focusing optical element 40 of the first resonator section 26 without greatly diverge. In any case, the beam radius or mode radius in this exemplary embodiment remains in the range of twice the value of the beam radius from the location of the laser medium 23. From FIG. 11 it can also be seen that, in the case of an embodiment according to the present invention, the beam stailie (= constriction) 41 (formed by the focusing optical element is) is not necessarily located at the location of the laser medium 23.
    In addition to the embodiments illustrated in FIGS. 3 and 8, further basic embodiments are possible, wherein more than one focusing optical element could also be provided in the first resonator section 26 (more than one crossing point of the beam axes 30, 30 'results can). Preferably, if the resonator has a plurality of crossing points 31, the laser medium 4 is arranged in the closest to one of the end mirror (the first end mirror in the illustrated embodiments) (or the pumping area of the laser medium 23).
    FIGS. 12 and 13 show by way of example two embodiments of coupled optical elements. For example, it may be the folding mirror 37, 39 or 36, 38 in the embodiments shown. In the embodiment of Fig. 12, the two optical elements are integrally formed with each other. In the embodiment of FIG. 13, the optical elements 37, 39 are rigidly connected to each other, here via a common base body 42, to which they are rigidly attached. In both cases, the optical elements are mounted together on a support part 43 of the resonator, preferably adjustable. A mounting part 44 for mounting on the support part 43 is indicated only schematically in FIGS. 12 and 13.
    The coupled optical elements, for example the folding mirrors 37, 39, have optical surfaces 45, 46 which have different centers of curvature. In other embodiments, different radii of curvature or different radii of curvature could be provided in combination with different centers of curvature. In still other embodiments, the optical surfaces of the coupled optical elements could be planar and lie in planes which are angled towards one another, preferably at an angle of more than 3 ° with each other. For example, one embodiment of such integrally formed optical elements could look like the base body 42 of FIG. 13 (without the optical elements 37, 39 attached thereto). * f * * * · »··« * «· · ·» »····························································« * '23 ........
    In further exemplary embodiments, of the coupled optical elements, these are, for example, the folding mirrors 37, 39, one having a curved optical surface and one having a planar optical surface.
    A similar tilting of the optical elements 37, 39 and 3ό, 38 about parallel tilt axes leads to opposite effects, for example, on the angular change of the output beam (at least the signs are opposite, the amounts may also be different). A common tilting of the optical elements 37, 39 or 36, 38 about an axis lying in the region of these optical elements, or their base body 42 or its mounting part 44 thus leads to an at least partial compensation of the associated effects.
    In addition to the already mentioned modes of the laser resonator, such as mode-locked resonator, Q-switched laser operation, operation as a regenerative amplifier, for example, an operation as a mode-locked and cavity-dumped resonator to achieve higher energies could be provided. «*
    Key to the reference numbers: 1 first end mirror 26 first resonator section 2 second end mirror 27 second resonator section 3 output beam 28 ABCD matrix 4 laser medium 29 output beam 5 folding mirrors 30, 30 'beam axis 6 folding mirror 31 crossing point 7 laser diode 32 folding mirror 8 optical element 33 laser diode 9 optical element 34 lens 10 optical element 35 lens 11 folding mirror 36 folding mirror 12 prism 37 folding mirror 13 prism 38 folding mirror 14 screen 39 folding mirror 15 laser medium 40 focusing opt. Element 10 first end mirror 41 beam waist 17 second end mirror 42 base body 18 folding mirror 43 support part 19 folding mirror 44 mounting part 20 folding mirror 45 optical surface 21 folding mirror 46 optical surface 22 Fa mirror 23 laser medium 24, 24 'first end mirror 25 second end mirror
    权利要求:
    Claims (18)
    [1]
    Patent Attorneys European Patent Attorneys European Trademark Attorneys Dl Herbert Hefel (until 2006) Dr Ralf Hofmann Thomas Rechner 6806 Feldkirch, Austria Egelseestr 65a, PO Box 61 Patent Attorneys · [] fj "HefelScHofmann 23291/33 / ss 100604 Patent claims 1. Laser with a laser medium (23) excited in a pumping area and a standing wave resonator optical element comprising a laser beam passing through a beam axis (30, 30 ') passing through the laser medium (23) and comprising first and second end mirrors (24, 24'; Resonator a first resonator section (26) having the first end mirror (24, 24 ') and optionally further of the optical elements (32, 40), with the laser beam between the first end mirror (24, 24') and the laser medium (23 ), And a second resonator section (27) having the second end mirror (25) and further of the optical elements (36-39) cooperating with the laser beam between the laser medium (23) and the second end mirror (25), in which at least one of the optical elements (24, 40) of the first resonator section (26) has a focussing configuration through which the beam axes (30, 30 ') of the laser beam which at respective tiltings of at least one of the second resonator section (27 ), at least one crossing point (31), and wherein this crossing point (31) or one of these crossing points (31) of the beam axes (30, 30 ') of the laser beam in the pumping region of the Laser medium (23) is or has a distance from the pumping area, which is less than the Rayleighlänge, which belongs to a portion of the laser beam between the laser medium (23) and the nearest focusing optical element (24, 40) of the first resonator section (26) is located, characterized in that the radius (w) of the laser beam at least over the portion of the laser beam, between the laser medium (23) and the nearest fok is less than five times, preferably less than three times, of the radius (w) of the laser beam in the pumping region of the laser medium (23) is lying element (24, 40) of the first resonator section (26). Bank details Österreichische Postsparkasse Account No. 92.111.622, bank code 60000 Swift code; OPSKATWW IBAN: AT55 6000 0000 9211 1622 Sparkasse der Stadt Feldkirch Account no. 0400-006300, bank code 20604 Swift code: SPFKAT2B IBAN: AT70 2060 4004 0000 6300 T +43 (0) 5522 73 137 F +43 (0) 5522 73 359 M office@vpat.at 1 www.vpat.at VAT ATU 65652215
    [2]
    2. Laser according to claim 1, characterized in that the radius {w} of the laser beam in the entire first resonator section (26) is less than five times, preferably less than three times, the radius (w) of the laser beam in the pumping area of the laser medium (23). is
    [3]
    3. A laser according to claim 1 or 2, characterized in that only one of the optical elements (24, 40) of the first resonator section (26) has a focusing training.
    [4]
    4. Laser according to one of claims 1 to 3, characterized in that the focal length of the laser medium (23) nearest focusing optical element (24, 40) of the first resonator section (26) is less than 100mm, preferably less than 50mm.
    [5]
    5. A laser according to claim 4, characterized in that the focal length of the laser medium (23) nearest focusing optical element (24, 40) of the first resonator section (26) is less than 20mm, preferably less than 10mm.
    [6]
    6. Laser according to one of claims 1 to 5, characterized in that the first end mirror (24) is a concave mirror.
    [7]
    7. Laser according to one of claims 1 to 5, characterized in that the first end mirror (24 ') is a plane mirror.
    [8]
    8. Laser according to one of claims 1 to 7, characterized in that the laser medium (23) nearest focusing optical element (24, 40) of the first resonator section (26) is a concave mirror.
    [9]
    9. Laser according to one of claims 1 to 8, characterized in that the resonator is folded by means of one or more folding mirrors (32, 36-39).
    [10]
    10. Laser according to one of claims 1 to 9, characterized in that the laser is a pulse laser, preferably a mode-locked laser.
    [11]
    11. Laser according to one of claims 1 to 10, characterized in that the radius (w) of the laser beam in the pumping region of the laser medium (23) is less than 250 pm, preferably less than 150 microns.
    [12]
    12. A laser according to any one of claims 1 to 11, characterized in that at least two of the optical elements of the resonator, which are arranged relative to the unfolded resonator at different distances from the first end mirror (24, 24 '}, are integrally formed with each other or rigid connected together and mounted together on a support part (43) of the resonator.
    [13]
    13. A laser according to claim 12, characterized in that the at least two integrally formed or rigidly connected and together on the carrier part (43) mounted optical elements optical surfaces (45,46) which are curved and have different centers of curvature and / or radii of curvature or which are planar and lie in angled planes to each other, or that of the at least two integrally formed or rigidly connected and mounted together on the support member 43 optical elements at least one curved and at least one has a planar optical surface.
    [14]
    14. A laser according to claim 12 or 13, characterized in that it is at the two at least two integrally formed or rigidly connected and together on the support member (43) mounted optical elements to two folding mirrors (36, 38, 37, 39), wherein the Laser beam between the deflections at these two folding mirrors (36, 38, 37, 39) of at least one further folding mirror (37, 38) is deflected.
    [15]
    15. A laser according to any one of claims 12 to 14, characterized in that the at least two integrally formed with each other or rigidly connected and together on the support member (43) mounted optical elements in a same direction tilting opposite effects on the displacement and / or the angular change of Beam axis (30) of the laser beam at another of the optical elements of the resonator or the laser medium (23) have.
    [16]
    16. A laser according to claim 15, characterized in that the at least two integrally formed with each other or rigidly interconnected and mounted together on the support member optical elements in a same direction tilting opposite effects on the displacement and / or the Winkelverände- tion of the beam axis (30 ) of the laser beam in an optical element of the resonator acting as an output coupler for the output beam (29).
    [17]
    17. Laser according to one of claims 1 to 16, characterized in that the laser is a solid-state laser.
    [18]
    18. A laser according to any one of claims 1 to 17, characterized in that the distance of the pumping region of the laser medium (23) from the nearest focusing optical element (24, 40) of the first resonator section (26) is less than three times the value of the Rayleighlänge the portion of the laser beam which lies between the laser medium (23) and the nearest focusing optical element (24, 40) of the first resonator section (26).
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    同族专利:
    公开号 | 公开日
    AT510116B1|2012-06-15|
    DE112011102088A5|2013-04-11|
    WO2011160143A2|2011-12-29|
    WO2011160143A3|2012-04-26|
    US20130089119A1|2013-04-11|
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    法律状态:
    2017-02-15| MM01| Lapse because of not paying annual fees|Effective date: 20160622 |
    优先权:
    申请号 | 申请日 | 专利标题
    ATA1031/2010A|AT510116B1|2010-06-22|2010-06-22|LASER|ATA1031/2010A| AT510116B1|2010-06-22|2010-06-22|LASER|
    PCT/AT2011/000219| WO2011160143A2|2010-06-22|2011-05-10|Laser comprising a laser medium|
    US13/806,026| US20130089119A1|2010-06-22|2011-05-10|Laser comprising a laser medium|
    DE112011102088T| DE112011102088A5|2010-06-22|2011-05-10|Laser with a laser medium|
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