SIDE-PUMPED LASERS

Abstract: Methods and apparatus for side pumping lasers are disclosed. By pre-collimating radiation emitted by laser diode arrays (62, 66), the present invention provides transverse mode matching to achieve fundamental, or TEM00, mode operation in the corresponding (nominally vertical) axis. Optics associated with the resonant cavity (106, 114, 110, 118) additionally redirect energy longitudinally through the gain media, enhancing fundamental mode operation in the (nominally horizontal) other axis as well. With dual forty-watt linear arrays of laser diodes (62, 66) and four longitudinal passes, TEM00 mode outputs exceeding fifteen watts have been achieved. By de-tuning the pumping radiation from the absorption peak of the lasing material (14) improved matching of pumping energy to the lasing volume is achieved.

Description: SIDE-PUMPED LASERS This invention relates to side-pumped solid-state lasers. Broad band arc lamps or flash lamps are often used to excite, or "pump," solid-state laser gain media. These lamps are typically positioned parallel to an elongated crystalline structure doped with a rare earth element such as Neodymium (Nd). Radiation emitted by these lamps is absorbed through the sides of the gain media with the Neodymium atoms absorbing the pump radiation and re-emitting it at the lasing wavelength or wavelengths characteristic of the given gain media. Surrounding or positioned adjacent the gain media of some relatively simple lasers are two mirrors. These mirrors act generally to form an optical resonant cavity through the gain media, redirecting the re-emitted radiation through the media until lasing results. Depending upon the configuration of the optical cavity, multiple modes of oscillation, or transverse electromagnetic modes (TEMs), may occur. Each TEM has a unique spatial characteristic within the resonant cavity, with the fundamental mode— TEM 00 ~both occupying the smallest volume within the cavity and having the lowest divergence. This mode additionally provides optimal focusing properties and displays a uniform Gaussian energy distribution across both the X (nominally horizontal) and Y (nominally vertical) axes. Operation in the TEM^, mode, accordingly, is desired for virtually all applications of pulsed and continuous wave (CW) lasers. Broad band arc lamps and flash lamps pump the entire gain media of the laser essentially indiscriminately. As a result, much of the pump energy that these lamps provide is directed to regions of the gain media outside the volume occupied by the TEMoo mode, not substantially contributing to amplification of the TEMoo laser beam but instead producing simultaneous oscillation of numerous TEMs and "mixed," or "multi"-mode, output. The efficiency of this pumping technique in converting pump light to the TEM 00 mode output is, therefore, relatively low. Laser diodes present more efficient pumping sources. Often configured so as to "end" pump the gain media, these diodes can be positioned so that their collective pump volume more closely matches that of the TEMoo mode. As noted in US-A-4908832 (inventor Baer - which patent is incorporated herein in its entirety by this reference), this end-pumping configuration of the diodes permits the pump direction to coincide with the longitudinal axis of the optical resonant cavity. It also limits the amount of energy that can be used and the resulting power of the laser, however; otherwise, power densities in the pump region of the gain media may become too great and produce heat exceeding that capable of being removed. Laser diodes may be used for side pumping gain media as well. As with broad band arc lamps and flash lamps, laser diodes may pump regions of the gain media outside the volume occupied by the TEM 0 o mode. In such cases devices such as spatial apertures can be used to eliminate much of the undesirable multi-mode output (see for example US-A- 4672616 - inventors Trost et al). Spatial apertures concurrently diminish the power output of the device, however, resulting in decreased performance and efficiency. Suitable diodes for side and end pumping gain media include those specified in the Baer patent and also are available from Laser Diode Products, Inc., 1130 Somerset Street, New Brunswick, New Jersey 08901. Additional techniques have been suggested to enhance the power output of these lasing devices. One proposed approach is to pump both ends of the gain media, while another is to utilise multiple gain media within the same cavity configuration. The ultimate power output available using these techniques remains limited by the amount of energy input to the individual pumping sites and the number of accessible sites, however. As the number of sites and gain media increase, these techniques become increasingly difficult to implement effectively. In the February 1, 1992 issue of Optics Letters, Messrs. Larry R. Marshall, A. Kaz, and R.L. Burnham mention a "three-pass oscillator" for a pulsed laser in an article entitled "Highly efficient TEMrø operation of transversely diode-pumped Nd.YAG lasers" (the "Fibertek article"). According to the authors of the Fibertek article, the fundamental mode path of the oscillator "traces a Z pattern through the gain volume," allowing "87% of the multimode energy to be extracted in the TEM^ mode." As shown schematically in Figure 3 of the Fibertek article, a single two-dimensional (i.e. stacked) array of laser diodes, at least some of which are connected in parallel, abuts the cylindrical Nd:YAG rod. The small-diameter (3.5 mm) rod thus necessarily collimates the diode radiation itself, limiting the volume of the fundamental mode. The small-diameter rod additionally cannot absorb all of the optical radiation directed into it from the stacked diode array, precluding the gain media from being pumped from more than one side. Although not addressed in the Fibertek article, the rod size further likely cannot support more than three passes through the gain media without degrading the TEM 00 mode output of the device. As a consequence of these (and other) limitations, the Fibertek article provides only "preliminary" experiments in connection with this technique. These limitations are also consistent with the results reported in the Fibertek article, which recounts higher outputs using a single-pass system having Brewster faces cut on the laser rod than with the Z pattern traced through the gain media. US-A-5257277 (inventors, Yagi et al) discloses a multi-pass laser comprising a plate shaped solid-state laser medium the edge of which is pumped by laser diodes. The plate shaped laser medium has a thickness less than the broadening width of the pumping light and a lens may be provided to improve absorption of the pumping radiation. The pumping light is confined within the laser medium by internal reflection and the laser beam fills almost the entire cross section of the laser medium. However such an arrangement allows higher modes than the TEM 00 mode to operate since diffraction effects caused by the difference in refractive index at the top and bottom faces of the plate shaped laser medium (the very type of effect relied upon by US-A-5257277 to provide total internal reflection) will encourage such higher order modes. Notwithstanding the disclosure of the Fibertek article and the Yagi patent US-A- 5257277 , there continues to exist a need for a scaleable, multi-pass pumping mechanism providing greater output energy than conventional end-pumping methods and more efficiency than existing side-pumping techniques. In lasers generally it is conventional wisdom that one wants if possible to match the pumping radiation to the peak in absorption of the laser medium so as to ensure maximum uptake of the pumping radiation. Good matching of pumping radiation is possible where lasers, such as laser diodes, are used to provide the pumping radiation and it is known, for example, to make lasers using a Nd:YAG laser medium (which has a peak in absorption at about 808.5nm) pumped with laser diodes emitting at 808.5nm. US-A-5048044 (inventor C.L.M. Ireland) discusses this need to match the pumping radiation with the absorption frequency of the laser medium and describes means that can be used to overcome the problems that result if the laser diode pumps drift off the absorption peak. These means comprise the provision of diffraction gratings or other deflecting means along the absorbing edges of the laser medium so that the pumping radiation makes many passes through the laser medium so extending the absorption path length. Such mechanisms are also discussed in US-A-5091915 (inventors Tatsumi et al) and in that document the provision of a longitudinally extending lens to focus pump radiation onto the diffraction grating is discussed. The present invention provides a novel laser giving high output in the TEMrø mode. The approach of the prior art is to match the physical volume of the laser medium to the desired lasing volume. In the present invention the lasing volume is a gain region within a larger volume of laser medium, only part of the laser medium being pumped. By using side pumping together with one or more collimating lenses, the present invention provides transverse mode matching to achieve fundamental, or TEM 00 , mode operation in the corresponding (nominally vertical) axis. Optics associated with the resonant cavity additionally redirect energy longitudinally through the gain medium, enhancing fundamental mode operation in the other (nominally horizontal) axis as well. The results are side- pumping techniques that not only are scaleable for greater rod lengths, but also are more efficient than conventional side-pumping methods. Accordingly the present invention provides a side pumped solid state laser comprising: a) a lasing material in the form of a body having a longitudinal axis; b) a source of pumping radiation; c) optical means to direct said pumping radiation transversely of the longitudinal axis onto the lasing material; and d) means for redirecting emitted laser radiation longitudinally along a plurality of paths through the gain region characterised in that e) the optical means is adapted to direct said pumping radiation onto part of the lasing material to define a gain region lying within the lasing material, the gain region being adapted to emit laser radiation and defining a folded TEM 00 mode volume having a height and width, the optical means being adapted to substantially match the height of the gain region with the height of the folded TEM o mode volume; and f) the means for redirecting the emitted laser radiation longitudinally through the gain region is adapted to substantially match the width of the folded TEM o mode volume to the width of the gain region. By lasing material is meant a material that emits laser radiation when stimulated under appropriate conditions. Embodiments of the present invention typically include a linear diode array positioned near each of the two sides of the gain media. A generally cylindrical lens associated with each array collects and collimates optical radiation emitted by the array, directing it into the gain media. The sides of the gain media themselves may be curved (confocally) to provide additional collimation, producing an excitation region within the media having an approximately rectangular cross section; this curvature also inhibits cross- lasing. Rather than solely employing spatial apertures to inhibit multi-mode oscillations in the horizontal axis, the present invention utilises multiple longitudinal passes through the gain media to discriminate against higher order modes. This discrimination, a form of "gain aperturing," occurs as the higher order modes—competing for the same physical space- overlap and effectively crowd each other to produce nulls or areas of low gain. In essence, the present invention "folds" the optical cavity within the gain media so that the TEM 00 mode volumes either are tangential or overlap only slightly, absorbing virtually all of the available gain. Experimental results using embodiments of the invention suggest that as few as two longitudinal passes through the gain media enhance this TEM 00 mode output. Using two linear laser diode arrays of forty watts each and four longitudinal passes have resulted in output powers exceeding fifteen watts in the TEM 00 mode. In these cases the "gain aperturing" achieved through the present invention effectively obviates the need for spatial aperturing, avoiding its associated losses entirely. Although useful for CW lasers, the present invention operates with Q-switched lasers and may be employed with quasi-CW, pulsed, and mode-locked lasers as well. In experiments involving acousto-optic Q-switching, output energies per pulse five times greater than those currently commercially available have been obtained. Because the diode arrays of the present invention are not positioned adjacent the ends of the rod, moreover, both the size of the arrays and the length of the gain media may be scaled to provide even greater output powers. Selected two-pass embodiments of the present invention have an optical cavity comprising an oblong Nd:YAG rod interposed between a "fold" mirror and a prism having highly reflective faces. A separate mirror is also optically coupled to the prism, as is an output coupler for the resulting laser beam. By inserting a suitable spatial aperture between the rod and fold mirror, TEM 0 o outputs of approximately three watts may be achieved in both the horizontal and vertical axes. Other two-pass embodiments omit the separate fold mirror, using instead a Nd: YAG rod having three faces at one end. Embodiments of the present invention supplying three optical paths longitudinally through the gain media similarly may include a fold mirror optically coupled to a highly reflective prism. These embodiments also comprise a second fold mirror coupled to the prism and substitute for the oblong rod described above one having three faces at one end. Although two of the faces reflect light incident at 45°, the third incorporates an anti-reflective coating for optical connection to the output coupler. Unlike the rudimentary disclosure of the Fibertek article, furthermore, the present invention neither employs multiple D-shaped (or semicircular) high reflectors nor positions such reflectors in the manner shown in Figure 3 of that article. Resulting fundamental mode outputs of the these three-pass embodiments currently exceed ten watts. Even greater output powers are achievable using the four-pass techniques of the present invention. The optical cavity of these embodiments includes an appropriate rod positioned between a prism at one end and a truncated prism at the other, each having highly reflective surfaces facing the bounded rod. A pair of fold mirrors are positioned opposite the sides of the prism, while a third mirror is optically coupled to a face of the truncated prism. Another face of the truncated prism is coupled to the output coupler to supply the resulting laser beam. Because this configuration produces virtually no TEM oscillation outside the TEMoo mode, no spatial aperturing need typically be employed. The invention also provides six-pass lasers and yet higher numbers of passes are envisaged. Because of the folded laser path the width of the gain region is wide in comparison with single pass lasers. This means that the laser can tolerate, and indeed performs better, if the pumping radiation is "detuned" from the absorption peak of the laser medium as this leads to the gain region being pumped relatively uniformly through its width. Such "detuning" of the pump radiation from the absorption peak is a technique that can usefully be employed in other multi-pass laser systems (it is not restricted to use in the TEM 00 systems of the present invention). Accordingly the invention further provides a side pumped solid state laser comprising: a) a lasing material having an absorption peak and in the form of a body having a longitudinal axis b) a source of pumping radiation tuned to emit radiation and arranged to direct radiation through the lasing material transverse to the longitudinal axis; c) means for redirecting emitted laser radiation longitudinally along a plurality of paths through the lasing material characterised in that:- the source of pumping radiation pumps at a selected frequency other than the absorption peak of the lasing material thereby improving the evenness of absorption of radiation across the lasing material. Other features, and advantages of the present invention will become apparent with reference to the remainder of the written portion and the drawings of this application. FIG. 1 is a perspective view of an optical cavity including a rod consistent with the present invention. FIG. 1A is a perspective view of one end of the rod of FIG. 1 illustrating the spatial volumes associated with various TEMs. FIG. 2 is a perspective view of a mechanism for transversely pumping the rod of FIG. 1. FIG. 3 is an end view of the mechanism of FIG. 2. FIG. 4 is a top plan view of a two-pass, side-pumped laser of the present invention. FIG. 5 is a perspective view of the optical cavity, including the rod and an optional spatial aperture, of the laser of FIG. 4. FIG. 5 A is a perspective view of one end of the rod of FIG. 5 illustrating the spatial volumes associated with various TEMs. FIG. 6 is a top plan view of an alternate embodiment of the two-pass, side-pumped laser of FIG. 4. FIG. 7 is a top plan view of a three-pass, side-pumped laser of the present invention. FIG. 8 is a perspective view of the optical cavity, including the rod and an optional spatial aperture, of the laser of FIG. 7. FIG. 8A is a perspective view of one end of the rod of FIG. 8 illustrating the spatial volumes associated with various TEMs. FIG. 9 is a top plan view of a four-pass, side-pumped laser of the present invention. FIG. 10 is a perspective view of the optical cavity, including the rod and an optional spatial aperture, of the laser of FIG. 9. FIGS. 10A-B are perspective views of the ends of the rod of FIG. 10 illustrating the spatial volumes associated with various TEMs. FIG. 11 is a top plan view of a four-pass, Q-switched, side-pumped laser of the present invention. FIG. 12 is a perspective view of the optical cavity, including the rod and an optional spatial aperture, of the laser of FIG. 11. FIG. 12A is a perspective view of one end of the rod of FIG. 12 illustrating the spatial volumes associated with various TEMs. FIG. 13 is a top plan view of a six-pass, side-pumped laser of the present invention. FIG. 14 is a perspective view of the optical cavity, including the rod, of the laser of FIG. 13. FIG. 14A is a perspective view of the ends of the rod of FIGS. 13 and 14. FIG. 15 is a graph of absorption v wavelength for aNd:YAG laser medium FIG. 16 is a schematic end views of a type of rod usable in the present invention FIG. 17 is a graph of power output v pumping frequency for a multi-pass laser in accordance with this invention. Illustrated in FIG. 1 is optical resonant cavity 10, including rod 14 of lasing material having ends 18 and 22. Rod 14 comprises an elongated crystalline structure, typically (although not necessarily) Nd:YAG, with ends 18 and 22 coated with material anti-reflective at the lasing wavelength. As shown in FIG. 1, rod 14 may have an oblong shape, with its respective top and bottom surfaces 26 and 30 being essentially flat and its respective first and second sides 34 and 38 having convex curves with anti-reflective coatings at nominally at the diode pump wavelength. The Neodymium (or other appropriate) atoms within rod 14 emit certain absorbed radiation at the lasing wavelength. Positioned adjacent end 18 is mirror 42, which reflects radiation emitted by the rod incident upon its surface. Adjacent end 22 of rod 14 is output coupler 46, through which the resulting laser beam 50 passes. Together, rod 14, mirror 42, and output coupler 46 form cavity 10, with the gain media incorporated within rod 14. If desired, spatial aperture 54 may be interposed between end 22 and output coupler 46 to filter the portion of beam 50 oscillating at other than the fundamental, or TEMoo, mode. FIG. 2 shows a mechanism, or assembly 58, useful for pumping the gain media of rod 14. In embodiments of the invention consistent with FIG. 2, assembly 58 comprises opposed arrays 62 and 66 of laser diodes. Each of arrays 62 and 66 contains a single row of multiple, series connected diodes 70 positioned to emit optical radiation toward rod 14. Although in some embodiments arrays 62 and 66 contain twenty-five diodes 70 (with adjacent diodes 70 placed approximately 0.085" apart), an important feature of the invention is that arrays 62 and 66 are scaleable: as the length of selected rod 14 increases, so too may the number of diodes 70 in arrays 62 and 66. Arrays 62 and 66 may be mounted on heat sinks 74 and 78, respectively, to remove excess heat generated by diodes 70 in use. Alternatively, integrated laser diode bars may be used in place of arrays 62 and 66. Positioned intermediate array 62 and second side 38 is lens 82. Generally cylindrical and with a radius of curvature " C > " lens 82 collects optical radiation emitted by diodes 70 of array 62 before directing it into the gain media of rod 14. Using known optical equations, R Q L and the distance D, between array 62 and lens 82 may be selected so as to collimate the light emanating from array 62. Depending on the respective diameters of lens 82 and rod 14, alternatively, lens 82 may make the radiation directed toward rod 14 slightly convergent as shown, for example, in FIG. 3. Lens 82, therefore, effectively "pre-collimates" the optical radiation directed toward rod 14. As a consequence, merely adjusting either or both of R QL and Oι enhances the vertical mode-matching ability of assembly 58 independent of rod 14. Lens 86 is similarly positioned intermediate array 66 and first side 34 of rod 14. Like lens 82, lens 86 is generally cylindrical and may be formed of fused silica or other glass. Lens 86 pre-collimates radiation emitted by diodes 70 of array 66, symmetrically directing the collimated light rays toward rod 14. As illustrated in FIG. 2, lenses 82 and 86 typically are at least as long as rod 14, ensuring that a substantial portion of the radiation emitted by diodes 70 is directed appropriately toward rod 14. FIG. 3 additionally shows a separate heat sink 88 to which rod 14 may be mounted. FIGS. 1 A, 2 and 3 detail the mode structure 90 of the gain media within rod 14 and cavity 10 when assembly 58 is used. First and second sides 34 and 38 of rod 14 are curved to provide additional redirection (or collimation) of the radiation emitted by diodes 70. The result is an excitation region 94 that has an approximately rectangular cross section. As best shown in FIG. 1 A, within excitation region 94 reside various TEMs of mode structure 90, with the space occupied by the TEM 00 mode centrally located therein. By pumping the sides 34 and 38 of rod 14 using arrays 62 and 66 and pre-collimating the optical radiation utilising lens 82 and 86, assembly 58 is effectively matched to the TEM 00 mode in the vertical axis. Consequently, the height H of excitation region 94 is approximately equal to the diameter of the TEMoo mode volume. By contrast, the width W of excitation region 94 is substantially greater than that of the fundamental mode, it not being matched to the mode volume. The lasing system 98 of FIGS. 4-5 counteracts the lack of correspondence between width W and the horizontal volume of the TEMoo mode. By passing optical radiation longitudinally through the gain media of rod 14 at different locations, effectively "folding" optical resonant cavity 102, additional regions of fundamental mode oscillations are formed. FIG. 5 A, for example, illustrates the mode structure 104 of system 98 at end 18 of rod 14, in which two regions 105 A and 105B of TEMoo mode oscillation (rather than one) appear. As a consequence, more of excitation region 94 is subsumed within the fundamental mode volume of rod 14, more closely matching that volume with the width W of the excitation region 94. In other words, system 98 of the present invention permits the TEMoo modes— whose volumes do not overlap— to experience greater gain in the (nominally) horizontal axis. It also causes higher order modes, which occupy larger volumes of space than the fundamental mode, to overrun (or "crowd") each other and themselves, thereby experiencing greater losses and lower gain. The result of this "gain aperturing" is increased output power of the fundamental mode. As detailed in FIGS. 4-5, optical cavity 102 of system 98 includes reflectors 106 and 110, prism 1 14, and output coupler 118 as well as rod 14. Reflector 106, whose reflective surface is slightly concave, is positioned adjacent end 22 of rod 14, while prism 1 14 may be placed adjacent opposite end 18. Together with reflector 110, reflector 106 and prism 114 provide a geometry supplying two longitudinal optical paths 122 and 126 through the gain media of rod 14. Because TEMs are associated with each of the two paths 122 and 126, two TEMQ O mode volumes are thus present. FIG. 5 A, as noted above, illustrates regions 105 A and 105B of TEM 00 mode oscillation at end 18 of rod 14. Similar regions exist at end 22 of rod 14, although the fundamental mode volumes at that end are more closely adjacent an imaginary centreline 130 of the rod 14. Prism 114 of system 98 may be a conventional right-angle prism having adjoining surfaces 134 and 138 that are highly reflective. Surface 134 is optically coupled to the reflective surface of reflector 1 10, while surface 138 interacts with output coupler 1 18 to provide the output beam 142 of the laser system 98. Reflector 106, in turn, functions as the vertex of the V-shaped paths 122 and 126. Suitable reflectors 106 and 1 10 may be obtained from Virgo Optics (a division of Sandoz Chemicals Corp.), 6736 Commerce Avenue, Port Richey, Florida 34668, and prism 114 is manufactured by, among others, Lightning Optical Corporation, 431 E. Spruce Street, Tarpon Springs, Florida 34689. If desired, spatial aperture 146 may be interposed between reflector 106 and end 22 of rod 14 to reduce the non-fundamental mode output of the laser. Consistent with the fact that the present invention is not limited to specific optical geometries, FIG. 6 illustrates an alternative embodiment of system 98. Unlike system 98, system 150 omits reflector 106 adjacent end 22 of rod 14, utilising an alternative rod 154 instead. Rod 154 includes opposed ends 158 and 162, with end 158 substantially similar to that of end 18. End 162, by contrast, is multi-sided, with faces 166 and 170 that are optically coated to be highly reflective to light incident at 45. In conjunction with prism 174 and reflector 178, faces 166 and 170 furnish optical paths 182 and 186 longitudinally through rod 154. Paths 182 and 186 result in the presence of two TEM o mode volumes, similar to those associated with paths 122 and 126. Because paths 182 and 186 are parallel (rather than V- shaped) within rod 154, however, the fundamental modes are substantially equidistant centreline 190 at both ends 158 and 162. Output coupler 194 presents the output beam 198 of system 150. FIGS. 7-8 show an exemplary three-pass, side-pumped laser 202 of the present invention. Prism 206 and reflectors 210 and 214 are coupled so as to provide longitudinal paths 218, 222, and 226 through the gain media of rod 230. As best illustrated in FIG. 7, paths 218 and 226 are essentially parallel through the gain media of rod 230, their connection at end 234 of rod 230 made because faces 238 and 242 are highly reflective to light incident at 45. Face 244 of end 234 is anti-reflectively coated to be transmissive, however, permitting light rays travelling along path 222 to exit rod 230 to output coupler 248. Reflector 214 is positioned so as to separate paths 222 and 226 within rod 230, providing, in the embodiment of laser 202 shown in FIG. 7, an angle A approximating 1. As with the other embodiments of the present invention, however, those skilled in the art will recognise that alternate geometries and components may be used if they produce satisfactory results. FIG. 8 again illustrates a spatial aperture 252 that may be used if other than multi- mode output is desired. FIG. 8 A, moreover, details the mode structure 256 of the gain media at end 260 of rod 230. As visible therein, some overlap of fundamental mode volumes 264 A, 264B, and 264C may occur. Together, however, volumes 264 A-C occupy a substantial portion of the width W of excitation region 268, further crowding, or reducing, the volumes otherwise occupied by the higher order modes. Although not shown in FIG. 8 A, as is apparent from FIG. 7 the mode structure at end 234 of rod 230 will include even less overlap among the fundamental mode volumes, subsuming yet additional space within the gain media. Four-pass laser 272 of the present invention (FIGS. 9-10) further enhances the fundamental mode output of the system. Resonant cavity 276 of laser 272 incorporates not only rod 278, prism 280, and reflectors 284, 288, and 292, but truncated prism 296 as well. These optical devices produce four longitudinal paths 300, 304, 308, and 312 through the gain media of rod 278, providing with output coupler 314 an output beam 316 composed almost exclusively of radiation in the TEMQQ mode. Thus, although FIG. 10 illustrates spatial aperture 320, that component is generally unnecessary to avoid substantial multi- mode output. Traced nominally from a point on path 312, radiation emitted by rod 278 in the fundamental mode may travel along that path to reflective surface 324 of truncated prism 296, where it is reflected onto the surface of reflector 292 and back to surface 324. From there, the radiation may travel through the gain media of rod 278 along path 312 to a first location 326 on reflective surface 328 of prism 280, reflecting from that surface to reflector 288. In reflecting the radiation, reflector 288 changes its direction an acute angle B, so that it encounters surface 328 at a second location 332 rather than first location 326. As a result, the radiation is thereafter reflected through rod 278 along path 308. After exiting rod 278 along path 308, the radiation contacts reflective surface 336 of truncated prism 296, redirecting it through rod 278 along path 304. Upon reaching first location 340 of prism 280, the radiation is reflected toward reflector 284 and redirected at an acute angle C to second location 344 of the prism 280. The radiation thereafter passes yet again through rod 278 along path 300 (parallel to path 312), reflected off surface 348 of truncated prism 296 to output coupler 314. FIGS. 10A and 10B illustrate the mode structures 352 and 356 present at ends 360 and 364 of the Nd:YAG rod 278. Mode structure 352 includes four non-overlapping TEM 0 o volumes 368A, 368B, 368C, and 368D that together occupy substantially all of the space available in excitation region 372. Clearly visible in FIG. 10A is the limited remaining space within excitation region 372~primarily in the center—available for higher order modes. FIG. 10B shows that the centre of excitation region 372 near end 360, moreover, is subsumed within TEM QO volumes 376A and 376B, further nulling the space available for higher order modes. Although fundamental mode volumes 376 A and 376B overlap, they thus nonetheless assist in suppressing non-fundamental mode oscillations. Also shown in FIG. 10B are TEMoo volumes 376C and 376D created by passing radiation along respective paths 300 and 312. Using a system of the present invention including a Nd:YAG rod 2.25" (about 57.2mm) long and 0.3" (about 7.6 mm) wide and about 3.8mm high an assembly 58 with diodes 70 collectively emitting eighty watts of radiation (i.e. forty watts per each array 62 and 66), the following results have been achieved: Number of Multi-mode (total) Fundamental Mode Fundamental Mode Longitudinal Passes output (watts) output (watts) %age of total 1 15% 1% 3% 2 15% 3% 20% 3 15% 10% 67% 4 18% 13% 72% Employing arrays 62 and 66 each emitting forty-five watts, furthermore, multi-mode and fundamental outputs of, respectively, twenty-seven and nineteen watts may be obtained with four longitudinal passes. The table clearly evidences the substantial benefits of employing the multi-pass systems of the present invention, which can provide more than twenty-five times the fundamental mode output of conventional single-pass lasers. For each of the one-, two-, and three-pass systems, a spatial aperture was utilised to filter the non-fundamental mode output. The four-pass system requires no such aperture, however, substantially depleting the non- fundamental mode output through the "gain aperturing" discussed above. Moreover, because the present invention does not inherently limit either the length or the diameter (width) of the doped rod, substantially longer and incrementally wider rods can be employed. Using a longer rod, for example, would permit additional radiation to be directed toward it using longer arrays 62 and 66, while utilising a wider rod would allow additional passes through the gain media without too much overlap of TEM 00 mode volumes. The present invention is not restricted to CW lasers, furthermore, but may be used with pulsed, Q-switched, quasi-CW, and other lasers as well. FIGS. 11-12 illustrate a four- pass system 380 similar to laser 272 and incorporating Q-switch 384. As those skilled in the art understand, Q-switch 384 can effectively block optical cavity 388 temporarily, employing radio frequency (RF) energy to change its refractive index as desired to provide a high-gain output of, typically, brief duration. Concepts such as frequency doubling and mode locking also may be practised in connection with the invention. FIGS. 13, 14 and 14A illustrate a six-pass design. Resonant cavity 400 comprises laser rod 402, truncated prism 404, 45° reflector 406, reflectors 408 410 and 412, and output coupler 414. Laser rod 402 has applied at one end reflectors 416 and 418 and has anti- reflective coatings in regions 420 and 422 . Laser rod 402 is 8mm across, 57.15mm long and 3.81mm high. Traced nominally from a point in region 420 on the end of laser rod 402, radiation emitted in the fundamental mode travels along path 430, is deflected by 45° reflector 406, reflected by reflector 408 and returned via 45° reflector 406 along path 430 to point 420. The radiation then passes through laser rod 402 (being amplified in the process) is reflected by an angularly disposed reflecting surface of truncated prism 404 and directed to reflector 410 from which it returns to laser rod 402 along a different path diverging slightly from its initial path from the laser rod. Because it is travelling a different path the radiation passes through laser rod 402 (again being amplified in the process) to reach reflector 416 where it is reflected to pass back through laser rod 402 (again being amplified in the process). Leaving laser rod 402 the radiation meets the end face of truncated prism 404 and is reflected back, again along a different path from which it came. The radiation passes through laser rod 402 (again being amplified in the process) to reach reflector 418 where it is reflected to pass back through laser rod 402 (again being amplified in the process). The radiation then meets a second angularly disposed reflecting surface of truncated prism 404 and is directed to reflector 412 from which it returns to laser rod 402 along a different path diverging slightly from its initial path from the laser rod. Following its last passage through laser rod 402 (again being amplified in the process) the radiation meets region 422 and travels on to output coupler 414 which is of conventional design. It is readily apparent that systems may be designed with higher numbers of passes but there are physical limitations. The first limitation is the depth in the laser rod to which the pumping radiation can reach. As mentioned above it is conventional in the art to match the pumping radiation with the absorption frequency of the laser medium. For a Nd:YAG laser medium (which has a peak in absorption at about 808.5nm) pumping is conventionally done with laser diodes emitting at 808.5nm. Control of this frequency is a problem as mentioned in US-A-5048044 referred to above. Reference is made to FIG.15 which shows the absorption coefficient for a Nd:YAG laser medium plotted against wavelength. The peak at 808.5nm absorbs more pumping radiation for a given rod width than 804.5nm however that does not mean more power out of a laser. When a laser is pumped not all of the pumping radiation is converted to laser radiation. Absorbed but "wasted" pumping energy gets converted into heat. Because radiation at the absorption peak is absorbed quickly the outer portions of a laser rod will therefore heat up more than the inner portions of the rod and this leads to several undesirable effects. Firstly, there is a limit on the amount of heating a rod can take without damage. Secondly the differential heating between inner and outer parts of a laser rod results in differing temperatures being present. As the refractive index of materials change with temperature this means that a "thermal lens" will result. The effect of such a lens is to focus the light away from the pumped regions resulting in a lower power output. By pumping off the absorption peak a greater penetration of the pumping radiation results which leads to a more even temperature distribution within the laser rod. Referring again to FIG.15 it can also be seen that the absorption peak at 808.5nm for a Nd:YAG laser medium is narrow. Much effort conventionally goes into trying to match that peak but it is narrow. However there are secondary peaks at 804nm and 806nm which merge to form a "shoulder" to the 808.5nm absorption peak. This "shoulder" is a broad target and absorption will not vary much across the shoulder. FIG.16 considers the situation for a four-pass laser in accordance with the present invention. Laser rod 700 is a rod usable in the present invention having a width of approximately 7.6mm and height 3.8mm. The beam diameter of the TEM o mode shown as 702, 703, 704, and 705 is approximately 1mm and the pumping radiation and pumped region of the laser is shown hatched. The rod is shown divided into four regions 712, 713,714,and 715 encompassing beams 702,703,704 and 705 respectively, each region having a width of 1.9mm. Tabulated below are calculated figures for the absorption in each region. These figures are rounded to the nearest percent and were calculated by measuring the total transmission of pumping radiation across the rod, calculating an absorption coefficient and then calculating the internal absorption based on the formula:- A=l-e αt where A = absorption α = absoφtion coefficient; and t = depth %age %age %age %age Total absorbed in absorbed in absorbed in absorbed in absorbed region 712 region 713 region 714 region 715 808.5nm 76% 19% 4% 1% 100% pumped from one side only 808.5nm 38% 12% 12% 38% 100% pumped from both sides 804.5nm 53% 25% 12% 5% 95% pumped from one side only 804.5nm 29% 19% 19% 29% 95% pumped from both sides It can be seen that pumping off the absorption peak results in a more balanced absoφtion of radiation through the laser medium. For the pumping at 808.5nm the absoφtion in the outer parts of the rod is more than three times that in the inner parts of the rod. For pumping off frequency this is reduced to 1.5 times that in the inner part of the rod. As the outer parts of the rod will lose heat faster than the inner parts this represents a considerable smoothing of the temperature profile of the rod across its width with consequent reduction in thermal lensing effects. It will be noted that pumping off the absoφtion peak also results in not all pumping radiation being absorbed. This reduction in absoφtion might be thought to reduce power but FIG.17 shows a graph of power v temperature for a four-pass laser such as that of FIGS. 9 and 10. The output frequency of a laser diode is dependant upon temperature. The laser diode pumps of the laser used in obtaining these results had an emission frequency of 808.4nm at 25°C which is its designed running temperature. For these laser diode pumps the emission frequency changes by about 0.3nm/°C. The graph shows higher power output for the pumping frequencies 804.5nm to 806nm over the power obtainable at 808.4nm. The running temperature of a laser diode depends upon designer choice and some manufacturers choose to run at lower temperatures than 25°C, for example 15°C, as some believe this prolongs the life of the laser diode. The applicant's invention of de-tuning the pumping radiation is therefore easily achieved with laser diode pumps where one may choose an "off the shelf laser diode pump and run it at a temperature other than its designed operating temperature; or one may select a laser diode having a suitable frequency at one's design temperature of choice. In effect, by de-tuning the pumping radiation from the absoφtion peak of the lasing material one achieves improved matching of the pumped region to the lasing volume. Clearly demonstrated is that the present invention, which combines transverse mode matching with multiple longitudinal passes through the gain media, achieves fundamental mode control in both the X and Y axes. Additional benefits accrue from use of a non- cylindrical, essentially oblong rod within the optical cavity, which optimises the shape of the excitation region for the multi-pass systems. The separate cylindrical lenses further enhance the mode matching achievable in accordance with the invention by pre-collimating the diode radiation independent of the rod itself. Their presence between the diode arrays and rod, unlike lasers in which an array abuts the rod, additionally permits defective diodes to be removed and replaced without disturbing either the rod or the alignment of the optical cavity and rod. Pumping at a frequency off the absoφtion peak of the laser medium results in an improved power output by reducing the chances of "thermal lensing". Thus, although the foregoing is provided for puφoses of illustrating, explaining, and describing embodiments of the present invention, modifications and adaptations to these embodiments will be apparent to those skilled in the art and may be made without departing from the scope or spirit of the invention.

Claims: What is claimed is: 1. A side pumped solid state laser comprising: a) a lasing material in the form of a body having a longitudinal axis; b) a source of pumping radiation; c) optical means to direct said pumping radiation transversely of the longitudinal axis onto the lasing material; and d) means for redirecting emitted laser radiation longitudinally along a plurality of paths through the gain region characterised in that e) the optical means is adapted to direct said pumping radiation onto part of the lasing material to define a gain region lying within the lasing material, the gain region being adapted to emit laser radiation and defining a folded TEM 00 mode volume having a height and width, the optical means being adapted to substantially match the height of the gain region with the height of the folded TEM 00 mode volume; and f) the means for redirecting the emitted laser radiation longitudinally through the gain region is adapted to substantially match the width of the folded TEM 00 mode volume to the width of the gain region. 2. A side pumped solid state laser as claimed in claim 1 in which the means for redirecting emitted laser radiation longitudinally along a plurality of paths through the gain region comprise a truncated prism having a plurality of reflective faces. 3. A side pumped solid state laser as claimed in claim 1 or claim 2 in which the means for redirecting emitted laser radiation longitudinally along a plurality of paths through the gain region comprise cut reflective faces at an end of the laser material. 4. A solid state laser as claimed in any of claims 1 to 3 in which the means for redirecting emitted laser radiation longitudinally along a plurality of paths through the gain region comprise reflective coatings applied to part of an end of the laser material. 5. A side pumped solid-state laser as claimed in any preceding claim in which the source of pumping radiation comprises a longitudinally disposed array of laser diodes. 6. A side pumped solid-state laser as claimed in any preceding claim in which the optical means to direct said pumping radiation transversely of the longitudinal axis onto the lasing material comprise a longitudinally extending lens disposed between the source of pumping radiation and the lasing material. 7. A side pumped solid-state laser as claimed in any preceding claim in which the sides of the body of lasing material are shaped to form a lens to at least partially collimate pumping radiation onto the gain region 8. A side pumped solid state laser comprising: a) a lasing material having an absoφtion peak and in the form of a body having a longitudinal axis b) a source of pumping radiation tuned to emit radiation and arranged to direct radiation through the lasing material transverse to the longitudinal axis; c) means for redirecting emitted laser radiation longitudinally along a plurality of paths through the lasing material characterised in that:- the source of pumping radiation pumps at a selected frequency other than the absoφtion peak of the lasing material thereby improving the evenness of absoφtion of radiation across the lasing material. 9. A side pumped solid-state laser as claimed in claim 8 in which the lasing material is a Nd:YAG material having an absoφtion peak at approximately 808.5nm and in which the pumping radiation is in the range 804.5nm to 806nm. 10. A side pumped solid-state laser as claimed in claim 8 or claim 9 in which the source of pumping radiation comprises a longitudinally disposed array of laser diodes having a designed operating temperature and selected to emit radiation at said selected frequency when run at said designed operating temperature. 11. A side pumped solid-state laser as claimed in claim 8 or claim 9 in which the source of pumping radiation comprises a longitudinally disposed array of laser diodes having a designed operating temperature and selected to emit radiation at the absoφtion peak when run at said designed operating temperature, the laser diodes being run at a temperature other than the design temperature so as to emit said selected frequency. 12. A side pumped solid-state laser as claimed in any of claims 1-7 in which the source of pumping radiation pumps at a selected frequency other than the absoφtion peak of the lasing material thereby improving the evenness of absoφtion of radiation across the lasing material.

Inventors: CRAMER LAURENCE E, HOBBS JOHN W, CRAMER, LAURENCE, E., HOBBS, JOHN, W.
Applicants: CRAMER LAURENCE E, HOBBS JOHN W, MORGAN CRUCIBLE CO, CRAMER, LAURENCE, E., HOBBS, JOHN, W., THE MORGAN CRUCIBLE COMPANY PLC
Application year: 1995
Main classification: H01S3
IPC codes: H01S3