More particularly, the invention relates to optically pumped compound planar waveguide devices and other solid state laser architectures that can be engineered to emit linearly polarized laser radiation from an optically excited isotropic lasing medium.

BACKGROUND OF THE INVENTION A common goal in laser systems is to provide devices with good beam quality that operate in an efficient manner. One technique for generating radiation having good transverse beam quality is to use a laser resonator that is relatively small in its transverse dimensions so that only diffraction limited or near diffraction limited transverse modes are supported by the resonator. In conventional rod-shaped laser resonators, this may be accomplished using pinholes or apertures in the laser cavity, or by only pumping or exciting a very limited transverse area in the gain medium. However, one drawback of this rod laser approach, in which only a limited transverse gain region is used, is that the small volume effectively limits the amount of energy that can be stored or the power that can be extracted by the laser system. In those cases in which pinholes are not used, but the excitation of the medium is limited to a small transverse area, one drawback is the difficulty encountered in designing an excitation source. In general, such small-excited volume systems use an end- pumping geometry in which a laser provides an excitation source to deliver the pump power into a well-defined region through the end of the laser rod. This approach similarly suffers from energy storage and extracted power limitations.

In laser resonators that extract high beam quality radiation from a transverse region that is large compared to that which would be required to support only a diffraction limited mode, it may be possible to use an unstable resonator. The

unstable resonator structure, however, exhibits high diffractive losses, and is thus limited in general to high gain laser systems.

Guided wave optics is largely based on the physical phenomenon of total internal reflection. It has important applications in the fabrication of miniaturized optical and opto-electronic devices where light radiation is confined within a defined region. An optical waveguide may be considered a light conduit consisting of a slab, strip or cylinder of dielectric material surrounded by materials with a lower refractive index. Optical dielectric waveguides are generally constructed of a guiding layer, a substrate and a cover layer. The guiding layer has a higher refractive index than the substrate and the cover layer to confine optical radiation by total reflection upon the walls separating it from the other two. Optical waveguides are discussed in "Fundamentals of Photonics"by B. E. A. Saleh and M. C. Teich (John Wiley 1991). In particular, a planar dielectric waveguide may be considered a conceptually simple two-dimensional design formed with a central slab of a medium of propagation with a higher refractive index. This guiding slab may also be described as a core. The upper and lower media of the structure are generally formed of a material with a lower refractive index. The lower medium may also be characterized as a substrate. When the upper medium has the same refractive index as the lower one, then the waveguide may be referred to as symmetrical. In addition, the upper medium may be simply surrounding air or another medium with a refractive index that is different from the substrate. The planar waveguide may be referred to as asymmetrical in these instances. A planar dielectric guide, however, generally does not provide confinement along the plane of the substrate. Dielectric strip or channel waveguides, which are also called three-dimensional guides, can provide this additional type of radiation confinement. Among strip waveguides, the most common includes those that are formed with a raised strip, an embedded strip and a rib or ridge or a strip loaded guide.

A waveguide laser generally includes a guiding layer with at least one lasant ion. By optically confining both the pump radiation and the developed

laser radiation to very thin structures, sufficient gain may still be generated from many ion-host combinations. The resulting gain, which may be offered by a particular waveguide configuration, enables a range of optical resonator designs that are conducive to producing near diffraction limited and diffraction limited output beams. For example, U. S. Patent 4,679,892 describes passive and active waveguide components and devices produced by liquid phase epitaxy and photolithography with garnet crystals of different refractive index. This technique may be particularly applicable to magneto-optical devices. In addition, U. S. Patent 5,502,737 describes the fabrication of waveguide laser structures by epitaxial growth of crystal layers from a liquid phase. Although this technique may be applied to the fabrication of planar waveguides, it imposes serious limitations on the choice of waveguide core and substrate material combinations due to lattice matching requirements for liquid phase epitaxy. To increase the refractive index of the guiding core, it may be necessary to co-dope the flux of it with ions such as Ga, Ge or Lu. This may undesirably alter the spectroscopic lasant properties of the core crystal, as by way of example manifested as line broadening. It may be necessary to match the crystal structure of substrate and guiding layers, thus making it particularly difficult to design waveguide lasers with a large numerical aperture that have the same desirable lasant characteristics as a bulk rod or slab laser. While waveguides of dissimilar materials such as single crystalline silicon on sapphire are known and have been used for the fabrication of modulators and switches, as described in U. S. Patent 4,904,039, analogous structures of guiding layers of dielectric crystals or glasses for solid state lasers cannot be grown in general, presumably because stresses between these dissimilar materials may not provide stable configurations.

Another waveguide approach includes the use of diode-pumped fiber lasers. In general, diode-pumped single-mode fiber lasers have demonstrated an ability to generate high beam quality laser radiation in which the diode pump radiation may be confined to a relatively large core as opposed to just the single- mode core that contains the active lasant material. This fiber approach has

generated a recent resurgence of interest for applications requiring output powers of 10 W or more. Although, in principle, such fiber lasers can be q- switched, they are limited in their peak power generation by physical processes such as Raman scattering. The Raman scattering threshold, which for single- mode fibers that are several meters in length is on the order of 10 GW/cm2, may limit the pulse energy and pulse widths that can be generated using the fiber laser approach. If this Raman threshold is exceeded, the laser output may be dominated by the Raman spectrum resulting in a broad super-continuum. This may be unacceptable for the majority of applications that require either single frequency or narrow band output pulses.

The operation of the first glass or crystal planar (non-fiber geometry) waveguide laser is open to interpretation depending specifically on how the thickness of a thin waveguide is defined. The early demonstration of a laser using a 50 m thick LiNdP4012 gain element, pumped by an Ar-ion laser, may be considered to be the first open literature report of the successful operation of a system that took advantage of and recognized the potential for planar crystalline structures. (K. Kubodera, J. Nakano, K. Otsuka and S. Miyazawa, A slab waveguide laser formed of glass-clad LiNdP4012, J. Appl. Phys. 49, pp.

65-68 (1978)). However, this initial demonstration employed a waveguide that was approximately an order of magnitude thicker than that which is generally required to support only single transverse mode operation in the waveguiding dimension. Furthermore, these waveguides were deposited by RF sputtering onto glass substrates and suffered from scattering losses. Since this initial demonstration, there have been many others using various laser systems to serve as pump excitation sources for various ion-host combinations. The most recent developments in the field of waveguide lasers have been associated with using semiconductor laser diodes as pump sources. Using such semiconductor pump sources, known pumping schemes for slab-type waveguide lasers have involved the use of coupling optics such as a spherical lens to focus a diode pump beam into the lasing core of the waveguide. The use of intermediate coupling optics between the semiconductor laser pump array and the waveguide core is

warranted in many of the developed systems by the highly divergent nature of the laser diode light. Because of the high divergence of the radiation emitted by a diode bar, there is a need to collect and collimate the light so that it can be delivered to the laser waveguide core with some efficiency. Typically, reported waveguide lasers use simple two layer, or three layer structures, in which the lasing core is either located on one side, or positioned between, a cladding material that has slightly lower index of refraction than the core. This step in refractive index is what permits the confinement of both the pump radiation and the developed laser radiation. One disadvantage of waveguide lasers with laser diode pump excitation sources is that the requirement of generating an output beam with high beam quality runs counter to the requirement of achieving simple and efficient pump laser radiation confinement. This conflict basically arises because in order to achieve efficient and simple pump confinement, it is often desirable to have a confining structure with a high numerical aperture, or in other words, a confining structure defined by an interface with a large step in the value of refractive index from one side to the other. The larger the numerical aperture of the waveguide, the larger the spread in angle of pump radiation that will be confined by the waveguide. However, a structure with a large numerical aperture will support a larger number of transverse lasing modes beyond the desired diffraction limited or fundamental mode than will a structure with a small numerical aperture. Because the spatial quality of a laser beam can be related to the number of transverse modes it contains beyond the fundamental mode, it is generally desirable to limit the numerical aperture that serves to confine the developed laser radiation. Because the same confinement structure is generally used for both the pump and the developed laser radiation, it is often necessary to compromise waveguide laser designs in current configurations given that both output laser beam quality and pump radiation confinement cannot be independently optimized.

In addition to providing improved laser beam quality and efficiency, it is often desirable to generate linearly polarized laser output. Linearly polarized output is often preferred for frequency conversion via harmonic processes, and

sum and difference frequency wave mixing in nonlinear optical crystals. Many solid state laser systems currently generate polarized output using either anisotropic crystals that are doped with laserable ions from the 3d series transition metals or the 4f series rare-earth ions, or similarly doped isotropic crystals used in combination with polarization selective optical components in the laser cavity. Some of the most common anisotropic crystals employed for use in solid state laser systems include lithium yttrium tetra fluoride (YLF) and yttrium vanadate (YV04). In addition, there are less common crystals such as strontium fluoroapatite (S-FAP) and lithium tetra fluoride (LuLiF). It has been observed that many of these anisotropic crystals cannot be grown readily in large boules, and are very expensive even in small sizes. Another aspect of their anisotropy is their inherent low strength that may be ascribed to their anisotropy, allowing cleavage and failure by fracture along specific crystalline planes. As one of the most common anisotropic crystalline laser media, YLF also suffers from low chemical durability in water-cooled systems. At the same time, YV04 is limited in its size and thermal properties, making it and YLF prone to thermal stress failure upon absorption of intense pump radiation.

Yttrium aluminate is another anisotropic lasing medium that, while not weak mechanically, is prone to twin crystal formation and much more difficult to grow than cubic YAG crystals.

Due to these and other detrimental properties, solid state laser (SSL) systems based on anisotropic crystals have limitations for commercial applications when high flux densities or high power requirements are involved.

Cubic crystals of the garnet family derive their wide acceptance and wider- spread use as SSL media from their strength, thermal conductivity, thermal shock resistance and availability as large crystal boules, and economical price and chemical inertness. They are the crystals of choice for high fluence and high power laser systems for commercial applications for their reliability and other useful features. Nd: YAG is the most commonly used laser crystal for SSL systems because it combines these properties in one crystal. The wavelength

that is most commonly used in Nd: YAG is the 4F3/2-4IIlX2 transition emitting laser radiation at 1.064 u. m. While this wavelength is useful, it is often desirable to up or down frequency-convert Nd: YAG laser radiation using nonlinear crystals for harmonic generators, or optical parametric amplifiers and oscillators for sum and difference frequency mixing. An inherent disadvantage of isotropic lasing media such as Nd: YAG is their laser output of random polarization which often has to be converted into linearly polarized output for electro-optical q-switching, frequency conversion and external modulation of the beam.

Another disadvantage of Nd: YAG laser rods in comparison to anisotropic crystals currently used is their tendency to suffer from induced birefringence due to thermal stresses. The induced birefringence can then result in depolarization losses effectively preventing Nd: YAG rods from reaching higher output powers due to this loss mechanism that is not encountered in anisotropic crystals. The thermal stresses generally cannot overcome their intrinsic anisotropic nature due to their crystal structure. The nature and origin of depolarization losses due to stress birefringence in Nd: YAG rods, and schemes of compensation are discussed for example in W. Koechner, Solid State Laser Engineering, Chapter 7 (Springer-Verlag, 1988). An acceptable approach however appears to be a 90° rotation with a quartz rotator located between two laser rods. But there are essentially no reasonable economical solutions that would eliminate insertion losses of rotator elements.

There also exists a need for a laser medium in SSL systems that would combine the mechanical strength advantages of isotropic crystals such as YAG with the polarized radiation generation advantages of anisotropic crystals such as YLF. More recent examples of engineered solid state laser materials are compound architectures of single crystalline or vitreous components, consisting of similar crystals. By way of example, U. S. Patents 5,441,803 and 5,563,899, and U. S. Patent Application Ser. No. 09/063,873 (which are incorporated by reference in their entirety as if recited herein) offer a possibility of overcoming

or reducing inherent disadvantages of conventional single component laser media such as ground state absorption losses of quasi-3-level lasing ions, and thermal lensing by adhesive-free bonding of single crystalline components into a configuration that possesses lasing properties that are unachievable by single component lasing media. Similarly, U. S. Patent Application Ser. No.

09/184,913 (which is incorporated by reference in its entirety as if recited herein) describes planar waveguide lasers that consists of 2,3,4 or 5 layered structures of laserable and non-laserable media to provide step changes in refractive index. An engineered laser material is thus desired to provide the aforementioned benefits without many of the known disadvantages including those described above.

SUMMARY OF THE INVENTION The apparatus described herein provide solid state waveguide lasers and amplifiers with high beam quality for a wide variety of commercial, military, and scientific applications. Various aspects of the invention may further provide a complete waveguide laser system that incorporate optical bonding techniques described herein to fabricate a crystalline or glass waveguiding laser medium. The laser medium may have a thickness appropriate for the generation and propagation of a low order transverse mode in the waveguiding dimension.

Furthermore, the invention may be modified to include laser diode pumping, q- switching, cooling, and packaging aspects of solid state waveguide laser systems.

An object of the invention is to provide a compound waveguide structure in which the developed laser radiation is confined by a waveguide structure that has a relatively smaller numerical aperture than another independent waveguide structure used to confine the pump radiation. The waveguide structure that confines the developed laser radiation may be independently modified from the waveguide structure that confines the pump radiation. The invention permits the independent optimization of laser systems to give high transverse mode output beam quality as well as efficient and simple pump radiation confinement.

Alternatives are further provided for designing and producing efficient and compact waveguide laser systems with high beam quality. Compound waveguides may be provided when dissimilar materials such as YAG and sapphire are bonded together. For example, a Yb3+ laser may be pumped at 940 nm and lasing at 1.03 um. The central layer may provide a lasing layer consisting of Yb doped YAG which has been fabricated from a bulk crystal.

Cladding on each side of the Yb: YAG layer may be formed as layers of undoped YAG which are also fabricated from bulk crystal. Because the Yb: YAG has a slightly higher refractive index than the undoped YAG, the interface between may confine the developed 1.03 llm laser radiation in a waveguide characterized by a small numerical aperture. Pump radiation confinement may be further defined by using two more layers, such as sapphire, on the outside of the YAG-

Yb: YAG-YAG structure. Because the refractive index difference between sapphire and undoped YAG is relatively greater than the refractive index difference between undoped YAG and Yb: YAG, the pump confinement waveguide has a relatively larger numerical aperture than the developed laser radiation confinement waveguide. The same basic waveguide structure may be applicable of course to many ion-host combinations beyond the Yb: YAG laser.

In particular, there are a multitude of choices for the lasing ion as well as the various layers that make up the waveguide. Additionally, the layers that make up the waveguide may be optically bonded together forming step changes in refractive index, and these various layers may also consist of different optical quality crystals or glasses. The components for each laserable waveguiding layer may originate from bulk crystals of defined properties, and remain unchanged in their desirable lasing parameters during the fabrication process.

Waveguide lasers formed in accordance with the invention may be laminated structures that function to generate laser radiation when optically pumped. Such waveguide lasers that are excited using laser diode arrays may have distinct and separate waveguide structures for confining the output radiation developed by the laser system independently from the pump radiation used to excite the laser system. The layers that comprise the waveguide structure may be composed of various optical quality glasses and crystals that are joined together using an optical bonding technology. Using optical quality glasses and crystals with different and appropriately chosen refractive indices in a given structure effectively provide and form the radiation confining waveguides. At least one of the layers in the waveguide structure may be doped with an active lasant ion that generates laser radiation upon being excited with pump radiation from a laser diode array. Because these waveguide structures confine both the pump and the developed laser radiation to a relatively smaller active volume, it is possible to develop and maintain high pump and extraction irradiances in the laser. This in turn provides many efficient laser systems having lasants that may conventionally be capable of developing only small gains. A multitude of oscillator and amplifier configurations are also compatible with the waveguide

structures provided herein, and of particular interest, these oscillator and amplifier configurations may lead to relatively high beam quality output laser radiation.

Another object of the invention is to provide a substantially planar compound waveguide lasing device. The device may comprise a compound five-layer planar waveguide positioned between two optically coated opposing surfaces configured for laser oscillator operation. The waveguide may include a central core layer consisting of a laserable medium with a refractive index n,, two inner laser-inactive cladding layers with a refractive index n2 wherein the core layer is sandwiched between the two inner cladding layers, and two outer laser-inactive cladding layers with a refractive index n3 wherein the core layer and the inner cladding layers are sandwiched between the two outer cladding layers. The respective refractive indices may be selected such that n, >n2>n3. An optical pump radiation source such as a laser diode may be further provided for transmitting pump radiation to the core and inner cladding layers to generate laser radiation output from the planar waveguide. The optical pump radiation may be transmitted through an anti-reflective optical coating. In addition, various layers of the compound waveguide may be formed with various dimensions and thicknesses, and may be joined with an optical adhesive-free bond such as a thermal bond. A cooling system in thermal contact with the planar waveguide may be also included for removing heat from the planar waveguide.

In yet another embodiment of the invention, a three-layer planar waveguide lasing device may be provided. The planar waveguide may be positioned between two optically coated opposing surfaces configured for laser oscillator operation having a core layer of laserable medium with a refractive index n,. A pair of planar cladding layers with a refractive index n2 may be also included wherein each individual cladding layer is positioned substantially adjacent to an external planar surface of the core layer, and where n, >n2. The lasing device may further include an optical pump radiation source for transmitting pump radiation to the core and inner cladding layers which

generates laser radiation output. The waveguide layers may be joined using an adhesive-free bond. The apparatus may also include cooling blocks for removing heat from the planar waveguide. In addition, the planar waveguide lasing device may further comprise a first and a second external layer formed of non-laserable material that are respectively positioned adjacent to exterior surfaces of the planar cladding layers. A multiple waveguide structure may be thus provided wherein a waveguide for confinement of developed radiation is formed by the interface between the core and inner cladding layers, and a pump radiation waveguide is formed by the interface between the inner cladding layers and either the non-laserable external layers or the surrounding environment.

An optically pumped solid state planar waveguide amplifier is further provided in accordance with the concepts of the invention. A planar medium capable of sustaining a population inversion may be centrally disposed along an optical axis formed along the direction of the incoming light rays. A pair of planar cladding layers may be separately bonded to the upper and the lower surface of the planar medium. The interface between the inner surfaces of the cladding layers and the planar medium may define a first waveguide by virtue of a first index of refraction discontinuity for spontaneous emission of the medium, and the outer surfaces of the cladding layers may also define a second waveguide by virtue of a second index of refraction discontinuity for containing radiation from the optical pump source. The amplifier may have coatings on its external surfaces that are anti-reflective to the pump radiation wavelength, and may include cladding layers joined with an adhesive-free bond. The two planar cladding layers may be formed of a first non-lasing dielectric medium.

Additionally, external layers formed of a second non-lasing dielectric medium may be positioned respectively adjacent to the outer surface of each planar cladding layer to provide a second waveguide by virtue of the index of refraction discontinuity at the interface between the first and the second non- lasing dielectric medium. The optically pumped waveguide amplifier may further include chill bars or other cooling systems in thermal contact with the amplifier.

The invention may further provide an optically pumped waveguide laser comprising a pair of reflective mirrors defining an optical cavity with an optical axis, and a planar waveguide disposed along the optical axis. The planar waveguide may include a gain medium layer and two planar cladding layers each defined by an inner surface and an outer surface. The inner surface of each cladding layer may be respectively bonded to the upper and the lower surface of the gain medium layer. The interface formed between the inner surfaces of the cladding layers and the gain medium layer may define by virtue of an index of refraction discontinuity a first waveguide for spontaneous emission of the medium. The outer surfaces of the cladding layers may define by virtue of an index of refraction discontinuity a second waveguide for containing radiation within the waveguide. The waveguide laser may further include laser diodes or other optical sources for providing pump radiation to the waveguide across at least one side surface of the planar waveguide. At least one reflective mirror can be mounted relatively external to the gain medium or formed as a monolith with the gain medium. Moreover, an external cylindrical lens may be positioned between the optical pump source and the planar waveguide. The apparatus may also have a first and a second external layer formed of a laser- inactive medium wherein the first and the second external layer is respectively positioned substantially adjacent to the outer surface of each cladding layer.

In accordance with yet another aspect of the present invention, solid state laser (SSL) systems are provided that employ an engineered lasing material effectively offering the laser designer a choice of lasing either with linearly polarized output or randomly polarized output. An object of the invention is to provide cubic crystals such as YAG based media, and vitreous or glass media, to emit linearly polarized output. Other objects of the invention provide waveguide laser components that can be engineered to emit linearly polarized output from an isotropic lasing medium, to modify the output laser beam profile by changing the refractive indices of the core and the inner cladding layers, and to substantially reduce parasitic oscillations. Another object of the present invention is to extend this engineered approach to SSL

systems for which polarized output is advantageous for frequency conversion of laser radiation, and generally, to high power laser systems with increased efficiency and improved beam quality. When isotropic cubic crystals or glasses are selected for waveguides and other solid state laser architectures, the invention described herein thus provides a choice between randomly polarized or linearly polarized laser output. Depending on fabrication conditions of compound formation with a dissimilar material, the lasing material may behave anisotropically during laser operation. This combination of crystals or glasses with a dissimilar material that is able to result in a stable bond preferably employs a configuration with the lasing medium sandwiched between two layers of dissimilar material but a compound of a lasing and a dissimilar non-lasing component also is operational. The term dissimilar refers to materials of different coefficients of thermal expansion. The compound formation between dissimilar materials can be engineered to result in the creation of a quasi- anisotropic lasing medium through the introduction of stresses that are formed into the system without negatively impacting the desirable thermal or mechanical properties of the originally isotropic laser medium. The lasing medium itself may also consist of a compound between similar crystals, such as for example, a doped garnet crystal of the YAG family, bonded in an adhesive- free bond to undoped YAG in an engineered configuration. The cladding material layer usually will consist of a single component but may itself also be formed from a compound structure. Compound SSL architectures that are operational in the present invention include waveguide lasers, rod lasers, slab lasers, microchip lasers and fiber lasers of glass or crystal compounds, and other architectures. These and other objects of the present invention will be explained in further detail below.

BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a simplified perspective illustration of a compound waveguide laser gain element formed in accordance with the invention that is configured to direct or confine pumped radiation within a central region.

Figs. 2-2A illustrate a planar compound waveguide consisting of five layers with shaped end surfaces that is positioned in proximity to semiconductor laser diode bars to provide an unstable resonator configuration.

Fig. 3 provides a perspective view of a compound waveguide laser gain element configured as a laser amplifier with laser diode bars positioned along the longitudinal sides of the waveguide.

Fig. 4 depicts a side pumped planar compound waveguide laser with a external mirrors that form the laser oscillator region.

Fig. 5 is an optically pumped waveguide laser with an output coupler that is configured as an external optic.

Figs. 6-7 illustrate various side pump configurations with one or more laser diode bars that can be used with waveguides formed in accordance with the invention.

Figs. 8-9 provide simplified end views of a side pumped waveguide having a cylindrical lens for directing laser diode pump radiation before its delivery to the waveguide structure.

Fig. 10 shows another waveguide pump configuration with a diode bar positioned in proximity to the end of the waveguide to direct pumped radiation.

Fig. 11 is a multi-layer planar waveguide with a cylindrical lens for directing pump radiation emitted by an end-mounted laser diode.

Fig. 12 is a simplified perspective of a thermal management system for a planar waveguide element.

Fig. 13 shows a cooling system or chill block positioned adjacent to a waveguide surface formed in accordance with the invention.

Fig. 14 provides a simplified perspective of another variation of the invention that includes a multi-layer waveguide formed with an external surface that is exposed to ambient surroundings.

Fig. 15 provides yet another embodiment that is a compound waveguide structure with an intermediate pump cladding region that approaches zero thickness.

Fig. 16 is an illustration of a waveguide structure having a top layer for confining pump radiation that is exposed to ambient surroundings.

Fig. 17 is a planar waveguide with an Nd: YAG core, two undoped YAG inner cladding layers, and two sapphire outer cladding layers collectively formed with generally canted sides.

Fig. 18 is a graph of calculated mode fields for the fundamental and first mode illustrating mode matching discrimination which strongly favors the fundamental mode.

Fig. 19 demonstrates operation in the fundamental mode with the core refractive index smaller than that of the inner cladding layer.

Fig. 20 is a simplified illustration of parasitic lasing modes in a waveguide laser structure.

Fig. 21 is a planar Yb: YAG waveguide laser with canted sides having a compound core consisting of a 15% Yb: YAG with two undoped YAG ends that provides lasing with linearly polarized output.

Figs. 22A-C are compound Nd: YAG rods consisting of a near- cylindrical Nd: YAG rod with two sapphire components adhesive-free bonded to it wherein the cross-section of the compound structure may be circular, elliptical, and with undoped ends; or a compound rod having undoped YAG ends with a central Yb: YAG lasing section, and a double-tapered contour.

Figs. 23A-B illustrates two variations of compound slabs formed in accordance with the concepts of the present invention that are capable of lasing with linearly polarized output which includes a compound Yb: YAG zig-zag slab with thick sapphire cladding, or a compound Nd: YAG slab with thin sapphire cladding.

Figs. 24A-B are compound microchip laser components with linearly polarized output that includes a high-power passively q-switched compound Yb: YAG microchip laser consisting of undoped YAG ends, Yb: YAG and Cr4+: YAG saturable absorber, which are adhesive-free bonded to each other, and with two sapphire side components; or alternatively, a compound microchip laser component consisting of Nd: YAG, Cr 4+: YAG which are adhesive-free bonded to each other, and to two sapphire sides components.

Fig. 25 depicts a compound glass structure preformed prior to redrawing into a compound fiber in accordance with another aspect of the invention.

DETAILED DESCRIPTION OF THE INVENTION The present invention provides compound waveguide structures for laser devices and optical amplifiers. The devices described herein are well-suited for many applications including high performance and compact laser and amplifier systems. A variety of output powers, ranging below 1 watt to several kilowatts or more, may be readily obtained by applying proper scaling techniques to the waveguide laser and amplifier structures described herein. It will be understood that the described features of the following embodiments may be considered individually or in combination with other variations and aspects of the present invention.

Fig. 1 illustrates a compound waveguide laser gain element 10 formed in accordance with the concepts of the invention. The planar structure 10 may consist of a number of relatively thin layers distinguished from neighboring layers in terms of their refractive index and whether active laser ions are present that are capable of generating laser radiation. The various layers within the waveguide structure may be formed of different glass or crystalline materials joined together at their interfaces using an optical bonding technology as described in U. S. Patent Applications Ser. No. 08/713,436 entitled SOLID STATE LASERS WITH COMPOSITE CRYSTAL OR GLASS COMPONENTS and Ser. No. 08/580,730 entitled COMPOSITE OPTICAL AND ELECTRO-OPTICAL DEVICES which are incorporated herein by reference. The waveguide 10 may include at least two separate pump and laser radiation confinement structures formed within the illustrated five-layer element having a central layer 12 and surrounding pairs of inner 14 and outer 16 cladding layers. The central layer 12 may contain active lasant ions for generating the laser radiation, and the interfacial surfaces on its top and bottom surfaces adjacent to relatively inner layers 14 may confine or direct the laser radiation developed within the central layer. The pair of relatively inner layers 14 may be positioned adjacent to the central layer 12, and the pair of relatively outer layers 16 may be in turn positioned adjacent to the inner layers. The relatively inner layers 14 may have an intermediate refractive index value in

between those of the central layer 12 and the two outer layers 16. At the same time, the central layer 12 may have the relatively highest index of refraction relative to all other waveguide layers. Laser diode array bars (not shown) may thus inject pump excitation radiation into a discrete pump region that at least includes the central lasing layer 12 and adjacent inner layers 14. With the existing differences in indices of refraction, the pump radiation may be confined to a pumped region defined by the interface formed between the inner 14 and the outer 16 layers, and the generated laser radiation may be confined within the substantially parallel central layer 12.

The refractive indices of the central 12, inner 14 and outer 16 layers denoted by n,, n2and n3, respectively, may be selected such that n, >n2>n3.

Furthermore, increased performance may be observed in particular applications when the step in index between levels as to the central layer 12 and inner layers 14, n,-n2, is relatively smaller than the step in index between levels as to the inner layers and outer layers, n2-n3. The waveguide devices described herein may demonstrate improved transverse mode quality output radiation in the waveguiding dimension (the relatively vertical dimension of the waveguiding element shown in Fig. 1) when the waveguide is designed to selectively support the fundamental mode in the waveguide dimension. The number of transverse modes that may be supported in the waveguiding dimension by the central layer is generally related to the thickness of the central layer and the index step between the central layer and directly adjacent layers such as the inner layers.

For example, when considering symmetric waveguides and transverse electric (TE) modes, the total number of modes that may be confined by the central layer of the waveguide structure is given by equation (1): where t, is the thickness of the central waveguiding layer, X is the vacuum wavelength of the radiation generated in the waveguide which is to be confined to the central layer, and INT means taking only the integer part of the expression

in the parenthesis. It may often be desirable to make the thickness of this central layer as large as possible, but not so large that it starts to let the next mode beyond the fundamental diffraction limited mode be confined. This may insure that only the diffraction-limited mode is supported by the waveguide structure and provide an output beam having relatively high beam quality in the waveguiding dimension. A reason for selecting a relatively high thickness for the central layer within the mode consideration limits just described may be generally related to the observation that the thicker the central layer, the more strongly the diode pump radiation is absorbed by the central layer. Using this criterion, a preferable thickness for the central layer may be represented by the following expression (2): Although the forgoing analysis is primarily directed for TE modes, there is an analogous treatment for other modes including transverse magnetic (TM) modes. TM modes may be generally characterized by a slightly weaker confinement than TE modes i. e., for equivalent mode numbers, and it has been observed that TM modes may be less confined than TE modes.

As shown in Fig. 1, the interfaces that define the confinement region of the pump radiation are distinct from those that define the confinement of the generated laser radiation. The step index which provides confinement of the pump radiation, n2-n3, may be independently selected or chosen as large as desired without regard to modal considerations of the generated laser radiation which is confined to the central layer. The pump radiation may be confined or limited to the central 12 and relatively inner 14 layers. Although it may be possible for higher order transverse laser mode to be contained within these three layers, this will not generally occur because of the higher gain experienced by laser radiation confined to the central layer 12 where the laser gain is located.

Choosing the step index between the inner 14 and outer 16 layers to be larger than the step index between the central layer and the inner layers can more

readily provide efficient confinement of the delivered pump radiation. In particular, the pump radiation may generally exhibit lower mode quality than the generated laser radiation in the central layer 12 because of relatively better confinement provided by the higher step index between the inner layers 14 and the outer layers 16 than between the central and inner layers. In addition, the numerical aperture (NA) of a waveguide provides a measure of the angular spread in radiation that may be confined by a waveguide. The NA may be defined as the sine of the half-angle of the radiation, measured external to the waveguide, which can be confined by the waveguide. Considering the interfaces responsible for confining the pump radiation, the NA of the pump waveguide may be given by equation (3): If pump radiation is directly emitted from laser diode bars in which the half- angle of the emitted diode radiation can be on the order of 30°, it is often desirable to provide a waveguide for pump confinement with an NA equal to sine (30°) = 0.5. For example, preferable waveguides defined by interfaces between undoped yttrium aluminum garnet crystals (YAG) and sapphire produce an NA value of 0.46 which has been observed to effectively confine laser diode array pump radiation.

A waveguide lasing device 20 formed in accordance with the concepts of the invention is shown in Fig. 2. The device 20 may include a five-layer compound planar waveguide element 25 positioned between two optically coated opposing surfaces configured for laser oscillator operation. The opposing surfaces may be end or side faces of the element 25, and may include either an optical coating or external mirrors. The optically coated surface may be monolithically formed with the waveguide 25 or provided on a discrete external optical element or mirror. The planar waveguide lasing device 20 may be configured as an unstable laser resonator for providing laser oscillation. The unstable resonator configuration may be obtained with or without a monolithic

confocal spherical resonator arrangement with spherical cavity faces.

Furthermore, the compound waveguide 25 may consist of a central core layer 22 consisting of a laserable gain medium with a refractive index n,. The laserable core 22 may be formed of a variety of materials capable of achieving population inversion to produce the lasing effect. In addition, the core layer 22 may be sandwiched between the two inner cladding layers 24 having a refractive index n2. Two outer laser-inactive cladding layers 26, which have a refractive index n3, may in turn sandwich both the core layer 22 and the inner cladding layers 24.

The differences of refractive indices between the various layers may be selected such that n, >n2>n3. As shown in Fig. 2, the lasing device 20 may further include an optical pump radiation source 28 for transmitting pump radiation to the core 22 and inner cladding 24 layers to generate laser radiation output. The optical pump radiation may be substantially absorbed in the core layer 22 in at most two passes through the waveguide 25. The waveguide 25 may be defined by at least two opposite side or end surfaces so that optical pump radiation from a source such as a laser diode enters and exits through these opposing surfaces of the waveguide. A variety of substantially anti-reflective optical coatings at the pump wavelength may be deposited onto the side surfaces of the waveguide 25 through which the pump light is transmitted in order to enable transversal pumping. The optical pump radiation may be transmitted to the waveguide sides in a direction perpendicular to the optical axis or the direction of propagation of the generated laser radiation 29. This selective passage of radiation at the pumping wavelength may be accomplished without the aid of intermediate lenses or fibers to at least one waveguide side. Alternatively, the optical pumping radiation may be transmitted through an optically coated end surface having dichroic properties that is anti-reflective or transmissive at the pump wavelength but reflective at the lasing wavelength. The pump radiation may be thus injected into the planar waveguide 25 in a selected direction that is either substantially perpendicular or parallel to the optical axis, or in the direction of propagation of the generated laser radiation.

The laserable medium 22 may include an optically inert host lattice and an optically active species. The refractive index difference between the laserable core layer 22 and the inner cladding layers 24 may be established by different crystallographic orientation of the same crystal host. For example, a variation of invention may include a central core layer with at least one laserable ion contained in yttrium aluminum garnet (YAG) crystal structure as a host lattice that is substantially sandwiched by inner cladding layers consisting of laser-inactive undoped YAG and outer cladding layers consisting of sapphire.

The laserable medium of the core layer may be formed of YAG doped with at least one ion or combination of elements selected from the group consisting of rare earth elements including Cerium, Praseodymium, Neodymium, Promethium, Samarium, Europium, Gadolinium, Terbium, Dysprosium, Holmium, Erbium, Thulium, and/or Ytterbium, and third-transition metals such as Chromium, Titanium, and Cobalt. In addition, the core layer 22 and the inner 24 and outer 26 cladding layers may be selected from fluoride single crystals.

The core layer 22 and the inner 24 and outer cladding 26 layers may be respectively formed of laser-active and laser-inactive fluoride, fluorophosphate, silicate or phosphate glasses. In a particular embodiment, the core layer may be formed of Cr2+: ZnSe and the inner cladding layers may be formed of ZnSe. The core may also include Crions admixed as laserable ions in an optically inert single-crystalline host lattice. Additionally, the central waveguide core 22 may include Cr4+ ions admixed to a laserable material resulting in passively q- switched laser operation. The core layer 22 may include a bonded segment of Cr4+: YAG located either on one end or in the interior part of the core layer. One or more sides of the segment may be in contact the central rare-earth doped YAG layer and sandwiched between undoped YAG pump cladding layers. The planar waveguide may be thus configured for passively q-switched lasing operation permitting the generation of short q-switched output pulses with pulse durations from approximately 0.5 to 50 nanoseconds. The central or laserable layer 22 may be thus formed as a compound core structure where all segments or portions may have a similar refractive index but are not all laser-active.

Selected component layers of the waveguide 25 may consist of glass with essentially similar viscosity, and may be joined with an optical or adhesive- free bond. Direct contact between various surfaces of the layers may be verified with optical measuring techniques. The bonding of the compound planar waveguide 25 may be also thermally assisted with controlled direct heating that does not necessarily rise to the level of diffusion temperature ranges. In particular, the core layer 22 may be optically bonded or directly bonded with thermal energy to the inner cladding layers 24. The waveguide 25 may be formed by thermal bonding from a preform structure that is thermally redrawn with proportionate cross-sectional dimensions. Moreover, the core layer 22 may be formed of variable thickness including a range from approximately 3-15 microns. The inner cladding layer 24 may each have a thickness range of approximately 5-15 microns, and the outer cladding layer 26 may each have a thickness range of approximately 200-4000 microns. Each layer may be formed with similar dimensions such as 1 cm in length and 5 mm in width. The planar waveguide lasing device 20 may further include a cooling system (not shown) that is in thermal contact with the planar waveguide for removing heat from the planar waveguide. Cooling bars or elements within the cooling system may be positioned substantially adjacent to or near the waveguide to effect heat transfer typically through convection, radiation or conduction. At least one advantage of the waveguide lasers provided herein over other conventional rod laser geometries includes the ease with which high-average-power thermal loads can be dissipated without incurring excessive temperature rises in the lasing medium. Generally, for uniformly heated structures, i. e., those in which the heat source is located uniformly throughout their volume, the center-to-edge temperature rise scales as the thickness of the volume to the second power. For example, a rod laser with radius r may have heat removed from the cylindrical surface of the rod, and the temperature rise from the center of the rod to its edge will scale as r2. In a waveguide laser, in which the heat generation is confined to the central layer containing an active lasant ion, the temperature rise across this layer generally scales as the thickness of the central layer to the second power,

i. e., t2. Because typical rod radii for 10 W to 100 W lasers generally measure from mm to cm, while the range of preferable waveguide central layer thickness of the present waveguides are generally on the order of 10 microns (0.01 mm), the temperature rise across the central gain loaded layer of the waveguide may be orders of magnitude less than the temperature rise across the radius of a comparable average power laser rod. In many laser systems where the temperature of the lasing material may be controlled to achieve efficient operation, this reduced temperature rise in the waveguides provided herein may provide particular advantages over other conventional rod laser geometries.

Problems relating to thermal distortions with waveguide lasers in general may be significantly reduced, and more aggressive thermal management may be available for quasi-three-level lasers and other systems that suffer from ground state reabsorption losses such as Yb3+, Tm3+, and Ex3+.

As shown in Fig. 2, two semiconductor laser diode bars 28 may operate as pump excitation sources juxtaposed adjacent to the sides of a waveguide 25.

The laser diode bars 28 may emit pump radiation directly into the central region or pump radiation-guiding portion of the waveguide 25. The sides of the waveguide laser 20 may have an applied anti-reflective optical coating at the pump wavelength to increase the coupling efficiency of the pump radiation into the waveguide. The waveguide crystal 25 itself may be configured with either spherical or cylindrical surfaces on each of its ends to form an unstable resonator in the unguided direction or other appropriate laser oscillator. The configuration may provide high beam quality laser radiation generated in the central layer 22 of the waveguide in both the guided and unguided dimensions.

The waveguide structure 25 itself may control the beam quality in the guiding dimension by allowing only a single or a small number of transverse laser modes to be confined in the central guiding or laser radiation layer 22. The unstable oscillator structure may also control the beam quality in the larger unguided dimension using principles that are well known to those of ordinary skill. Optical coatings may be directly applied to waveguide ends to form a monolithic resonator structure which includes the application a high-reflective

optical coating on one end, and a partially reflective optical coating on the other end of the waveguide. Various configurations for the optical coating on the output end of the laser waveguide may be of course selected such as dot reflectors or graded reflectivity coatings in order to enhance beam quality in the unguided dimension. In situations where high mode quality may not be required in the transverse or unguided dimension, ordinary stable oscillator configurations may be employed.

The diode bars 28 in Fig. 2 may be located along the side of the waveguide laser 20 to permit their emission of pump radiation directly into the central region of the waveguide consisting of the central 22 and inner 24 layers.

High beam quality may be achieved by using one ore more laser diode array bars as sources that inject pump radiation into relatively thin planar structures consisting of glass or crystalline materials. Because the waveguide laser 20 may confine both the pump radiation and the developed laser radiation, it may be possible to develop high gains that permit the use of an unstable resonator in the non-guided direction. Unstable resonators in one dimension are also known as strip unstable resonators, and are known in the field. In Fig. 2, the unstable resonator, also known as a confocal unstable resonator, the internally extracted laser beam is collimated as it travels away from the high reflector (HR) end 21 of the laser cavity and toward the output coupler (OC) end 23 of the cavity.

With confocal unstable resonators, the radius of curvature of the high reflector is related to the radius of curvature of the output coupler and the axial length of the resonator structure by expression (4): -oc=2/(4) where RHR and Roc are the radii of curvature of the HR and OC, respectively, l is the cavity length, and the orientation of the end face curvatures are as shown in Fig. 2. The laser diode bars 28 pump the waveguide structure 25 through its sides which may include an anti-reflection coating at the pump wavelength to increase the transmission of the pump light into the laser cavity. The output

beam may be emitted from the output coupler end 23 of the waveguide structure 25.

In accordance with another embodiment of the invention, a waveguide oscillator design may be selected for generating 10 W of output radiation at 1.029 um using pump diodes at 940 nm. The central laserable layer may be composed of 15 atomic % Yb3+: YAG with refractive index 1.821, and may have a thickness of approximately 6 m. By using the given index values for the central layer and the inner pump cladding layers, application of equation (2) yields 6.03 pm as the maximum core thickness that may still preclude the lasing of the next mode above the fundamental mode in the waveguide dimension.

The inner pump cladding layers may be composed of undoped YAG with a refractive index of 1.819, and would also be 6 pm thick. The outer layers may be composed of sapphire with a refractive index of 1.76. With these index values, the diode pump light may be confined by a waveguide having a NA of 0.46, which means that it may capture light emitted from the diode bar at up to 27.3 ° from the optic axis. This may permit efficient capture of radiation emitted from laser diode bars without the need for any intermediate coupling optic.

Fig. 2A describes another waveguide structure 20'that may be formed in accordance with the invention for developing high beam quality radiation in the non-guided dimension with an unstable resonator architecture. The unstable resonator is a confocal design in which the radii of curvature of the output coupler and the high reflector satisfy equation (4), and the intracavity laser beam traveling toward the left in Fig. 2A, i. e., toward the output coupler, is collimated. By using two 10 W cw 940 nm pump diode bars, a simple energetics model of the system suggests a greater than 10 W of cw output power using an effective output coupler reflectivity of 33%. The cavity may have a geometric magnification of 1.5, which means the desired effective output coupling reflectivity of 33% can be realized by coating the central 3.33 mm of the 5 mm wide output aperture with a coating 27 having a reflectivity of 50% at

1.03 nm, and coating the remaining outlying portion of the output coupler aperture with a coating that is anti-reflective at 1.03 nm.

While these waveguide lasers employ the difference in refractive index between doped YAG as a core layer, undoped YAG as a cladding layer for cladding pumping, and sapphire as a substrate, many other combinations are possible. Among other useful combinations, in general, there are doped oxide or fluoride crystals that may provide a core, undoped oxide or fluoride crystals as a cladding layer, and different crystals or glasses of appropriate refractive index as substrates. In situations where the difference between doped and undoped uniaxial crystals, especially at low dopant levels, is not sufficient for proper waveguiding operation, the difference in refractive index between the ordinary and extraordinary crystallographic orientations may be exploited.

Similarly, choosing available optical glasses of different refractive index may allow the construction of a waveguiding device according to the invention. Yet another embodiment includes the use a lutetium-analog of an yttrium based laser host crystal for both the doped and cladding layers, and undoped yttrium crystal as the substrate. For example, doped LuLiF, undoped LuLiF and YLF layers can be designed for waveguide lasers described herein. Applying these design principles may result in providing waveguide lasers with laser active ions of the 3d and 4f transition metal ions in single-crystalline oxide and fluoride laser host lattices, and in any of the laser glasses of interest, especially phosphate, silicate, fluorophosphate and fluoride glasses.

Another variation of the described waveguides laser may include a segmented core. Two ore more core sections may be joined with a laser- inactive segment of essentially similar refractive index to allow for space requirements and efficient placement of many commercially available laser diode bars for side pumping. This type of arrangement may provide practical solutions for scaling waveguide lasers to higher powers and avoiding unpumped core areas which, in turn, may give rise to ground state absorption losses of quasi-3-level laser systems. In addition to providing segments between laser- active core sections, laser-inactive or saturable absorber sections may be placed

at the ends of at least one of the core sections, for instance, to provide waveguiding of input or output radiation. Another variation of the invention provides a waveguide structure with an undoped guiding core. This core may have a cross section of 10 llm x 10 m, and may further include cladding layers of laserable material surrounding it on its four sides, with a thickness of the cladding layers of 15 um each. The core may of course be formed with other configurations that may be surrounded by one or more cladding layers. One end face of the waveguide component may be coated uniformly with a high- reflectivity (HR) dielectric coating. The second end face may be selectively HR coated over the clad regions while the core has a coating deposited on it that serves as output coupler for the generated laser radiation. In another variation of this design, the core section may be recessed from the end face by 0.5 mm, and thereby readily differentiable in terms of coating deposition. The undoped guided core of an originally uniformly HR coated end face may be also selectively ion milled to produce an output coupler coating over its surface.

This configuration of a waveguide laser may provide a purely diffraction limited output by collecting laser radiation generated in the doped cladding and retaining only the diffraction limited portion.

The compound waveguide gain elements described herein may be readily configured as an amplifier 30 as shown in Fig. 3. The gain element 35 may consist of five layers and have two adjacently positioned semiconductor laser diode bars 38 that serve as pump excitation sources. In addition to using these waveguides 35 in laser oscillators, they can also be used as amplifiers where an incoming optical beam 32 is aligned to pass through the central portion of the waveguide structure 35 and under go amplification as it traverses the structure. The laser diode bars 38 may be positioned substantially adjacent to the sides of the waveguide 35 for their injection of pump radiation into the pump radiation-guiding portion of the waveguide. The sides or ends of the waveguide 35 may of course include anti-reflective optical coatings at the pump wavelength to increase the coupling efficiency of the pump radiation into the waveguide. Optical coatings that are anti-reflective at selected wavelengths may

be applied to any surface in which the laser beam enters and exits in an effort to increase the efficiency of the amplification process. Furthermore, the ends of the waveguide amplifier 30 may be planar or any other curved or linear configuration. The laser radiation to be amplified 32 may be incident on one end of the amplifier 30, and after traversing the central portion of the amplifier, the amplified laser radiation 34 may exit at the opposite or other end of the waveguide structure 35. The compound waveguides described herein provide an improved technique of coupling pump radiation into the waveguide containing the gain medium. When configured as either a waveguide amplifier or laser, the additional confinement layers create another guided layer in addition to that containing the gain medium. The plurality of additional guiding layers may serve to efficiently confine pump radiation, and more effectively pump an active or laserable region within a gain medium. These compound planar waveguide structures further allow for the capture of energy that may be emitted at high divergence angles by laser diode bars, and the confinement of that energy into a waveguide containing the gain medium. These improved pumping schemes may thus generate relatively high gain in the gain media. For compactness, the dimensions of the gain media may also be small relative to those of standard devices. The conventional single-mode fiber or rectangular waveguides may be scalable but generally leads to drastically extended waveguide lengths. Meanwhile, with the planar waveguide geometry adopted herein, the spectral and spatial coherence of the device output may be controlled both by the waveguide and resonator configuration. In applications were the spatial coherence afforded by the waveguide is insufficient, the high gain may allow for the use of an unstable resonator. The compound waveguides provided herein may be formed of layers of materials with selected optical properties, and may be bonded together thermally, optically or otherwise, from layer to layer along their relative interfaces to provide a structure that is relatively strong enough to undergo further finishing processes and withstand other demands placed upon it by subsequent formative and fabrication methods.

Another variation of this embodiment may provide an optically pumped solid state planar waveguide amplifier formed with a substantially rectangular shape or any other desired configuration. The amplifier may include a planar medium that is capable of sustaining a population inversion. The planar laser medium may be centrally disposed along an optical axis formed along the direction of incoming light rays, and may include an optically inert host lattice and an optically active admixted species. At least two planar cladding layers with an inner surface and an outer surface may be positioned adjacent to the planar medium wherein the inner surface of each cladding layer is respectively bonded to the upper and the lower surface of the planar medium. The interface between the inner surfaces of the cladding layers and the planar medium may define a first waveguide by virtue of a first index of refraction discontinuity for spontaneous emission of the medium. The planar medium may be a solid state medium and the cladding layers may be formed of a non-lasing dielectric medium. These and other layers within the amplifier may be joined with an adhesive-free bond such as those provided by thermal or diffusion bonding techniques. Moreover, the interfaces forming the first waveguide may have a discontinuity in the index of refraction due to birefringence in a common crystal. The first waveguide may have a substantially single transverse EM mode by virtue of the ratio of transverse dimension of the first waveguide relative to the wavelength of the stimulated emission of the amplifier, or the difference in indices of refraction across the defining interface of the first waveguide. The outer surfaces of the cladding layers may further define a second waveguide by virtue of a second index of refraction discontinuity for containing radiation from the optical pump source. A first and a second external layer formed of a second non-lasing dielectric medium may be also thermally bonded or otherwise joined to the outer surface of each cladding layer. The second waveguide may be provided by virtue of the index of refraction discontinuity at the interface between the first and the second non-lasing dielectric medium. The second waveguide may also have an acceptance angle greater than or equal to the divergence angle of the optical pump source.

Additionally, the amplifier may be configured to receive pump radiation from a pump source that is substantially perpendicular or parallel to the optical axis. A variety of optical coatings may be applied to various external surfaces of the amplifier that are anti-reflective or reflective to the pump radiation wavelength.

As with other waveguide laser systems described herein, the optically pumped waveguide amplifier may further include a cooling system with chilling bars or blocks that are in thermal contact with the amplifier.

Fig. 4 provides another illustration of a compound planar waveguide laser 40 with separate mirrors. A high reflector 42 and an output coupler 44 may be selected for the laser oscillator. The end faces of the waveguide 45 may also have an applied anti-reflection coating at the wavelength of the generated laser radiation to improve the overall efficiency of the system by reducing intracavity losses. This oscillator structure is not monolithic, and includes stand alone discrete optics which serve as its output coupler 44 and its high reflector 42. The non-monolithic features of this embodiment may be of course applied to other variations of compound waveguides described herein.

Yet another embodiment of a laser oscillator 50 is depicted in Fig. 5 that is formed in accordance with the invention. This waveguide may be considered to have a hybrid or intermediate configuration between a monolithic structure (as shown in Fig. 1) and another having external discrete optics (as shown in Fig. 4). The high reflector 52 may be monolithically applied directly to the waveguide structure 55, and the output coupler 54 may stand alone as a discrete optic or external mirror. In this configuration, the high reflector 52 of the waveguide laser 50 may be of course formed by a highly reflective coating at the wavelength of the generated laser radiation 59.

Figs. 6-7 illustrate additional pump configurations that may be used with the planar waveguide lasers provided herein. One or more laser diodes 68 may pump radiation 62 directly into the pump guiding region 66 of the waveguide laser 60 from the direction of the waveguide sides 61 and 63. By juxtaposing two laser diode bars 68 to the sides 61 and 63 of the waveguide, as shown in Fig. 6, the pump radiation 62 may be transmitted into and confined within the

central pump waveguide region 66 consisting of the central 69 and inner cladding 67 layers. An increase in the coupling efficiency of the laser diode pump source 68 to the waveguide structure 65 may be observed when the sides 61 and 63 of the waveguide structure also include an anti-reflection coating 79.

The placement of the laser diodes 68 may be of course varied with respect to the waveguide 65 along different portions and distances away from the structure.

The planar waveguide lasing device 60 may consist of a three-layer pump waveguide that includes two optically coated opposing end faces or surfaces 61 and 63 configured for laser oscillator operation. The waveguide 65 may have a core layer 69 formed with two opposite external planar surfaces consisting of a laserable medium with a refractive index n,. In addition, two laser-inactive inner cladding layers 67 with a refractive index n2 may be each positioned substantially adjacent to an external planar surface of the core layer 69. The refractive index of the central layer 69 may be greater than the cladding layers 67 (nl>n2). The exterior surfaces of the inner planar cladding layers 67 may be additionally sandwiched by or positioned relatively adjacent to a first and a second external layer 64 formed of non-laserable material with a refractive index of n3 wherein n2>n3. An optical pump radiation source 68 may be further selected for transmitting pump radiation 62 to the core 69 and inner cladding 67 layers to generate laser radiation output from the planar waveguide 65. The received optical pump radiation 62 may be absorbed in the core layer 69 in at most two passes. All or some of the layers of the waveguide may be joined with an adhesive-free bond using as optical or thermal bonding techniques described herein. In addition, the planar waveguide lasing device 60 may further include a cooling system (not shown) positioned substantially adjacent to the planar waveguide 65 for removing heat from the apparatus. The cooling system may include cooling blocks, bars or other heat transfer elements. Fig. 7 illustrates another variation of the invention that includes a single laser diode bar 78 for directing pump radiation 72 into a selected side 73 of the waveguide structure 75. In addition to double or multiple-sided pumping, radiation may be also coupled or directed into a single side or end of the waveguides described herein.

In this configuration, pump efficiency may be improved by applying an optical coating 76 that is highly reflective at the pump wavelength to the side 71 of the waveguide structure 75 that is opposite to the diode pump source 78. This may allow the diode pump radiation or light 72 to be effectively double-passed through the waveguide structure 75. In addition, an anti-reflection coating 74 may be applied to the side 73 of the waveguide structure 75 which serves as the input surface to further increase the coupling efficiency of the laser diode pump source 78 and the waveguide 75.

As shown in Figs. 8-9, one or more cylindrical lens 84 and 86 may be used to collect and direct the diode pump radiation 82 emitted by laser diodes or pump sources 88 into a planar waveguide structure 85. Although light 82 from a laser diode bar or pump source 88 may be directly coupled into the waveguide 85, it may also be convenient to use intermediate optics 84 and 86 between the diode bar and the waveguide structure. A cylindrical lens or microlens 84 and 86 may both collect and collimate the diode light 82 prior to its injection into the waveguide pump region 87. By applying this scheme to the compound waveguides described herein, the divergence angle of the pump light delivered into the waveguide structure may be decreased or otherwise varied. A more efficient pump coupling with the waveguide may be accomplished with a pump confining structure that has a lower NA than if intermediate coupling optics are not used. Intermediate pump coupling optics may further allow the laser diode array to have a greater range of standoff distances from the waveguide structure.

The size and configuration of the pump coupling optics 84 and 86 may of course vary according to selected applications.

Additional pump configurations may be selected for delivering pump radiation to the compound planar waveguide structures described herein as shown in Figs. 10 and 11. As shown in Fig. 10, a single diode bar 108 may emit pump radiation 102 that is directly coupled or directed into the pump guiding region 107 through the end of a compound planar waveguide 105. By juxtaposing at least one laser diode bar 108 next to the end surface 101 of the waveguide 105, the pump radiation 102 may be transmitted into and confined to

the central region 107 of the waveguide structure 105 comprising a central laserable core 104 sandwiched between adjacent cladding layers 106. The waveguide end through which pump radiation 102 is transmitted may also include a high reflector in the laser cavity, and may have a dichroic optical coating applied to it. The optical coating may be highly reflective at the wavelength of the generated laser radiation, but transmissive at the wavelength of the pump radiation. As shown in Fig. 11, a cylindrical lens 114 may be further provided to first collect and direct the diode pump radiation 112 emitted by the laser diodes 118 before it is delivered into the waveguide structure 115.

As with other side pumping configurations described herein, it may be preferable in particular situations to include an intermediate coupling optic 114 between the laser diode bar 118 and the waveguide structure 115. Any combination of side and/or end pump configurations by one or more sources may be selected so waveguide structures provided in accordance with the invention may be pumped from multiple or different directions. For example, a substantially rectangular planar waveguide may be side pumped and end pumped together so pump radiation is introduced into the compound waveguide from three of its sides simultaneously or in a time controlled manner. Laser diode pump lasers may be configured to emit radiation at a wavelength that is absorbed by the dopant ion used as the active lasant in the waveguide to provide a laser oscillator. One or more intermediate optics may be positioned between the waveguide and pump radiation sources, and selected reflective and anti- reflective coatings at predetermined wavelengths may be further added to waveguide side surfaces. The waveguide may further include monolithically applied reflectors or separate and discrete optical components. These planar waveguides may be of course formed with a variety of geometric shapes and configurations as with other structures described herein.

Fig. 12 illustrates a thermal management system that may be selected for the described planar waveguide architecture. Two chill bars or cooling blocks 122 may be placed in thermal contact with the top 124 and the bottom 126 surface of the waveguide 125 through which the heat generated in the laser is

extracted. The proximity between the cooling elements 122 and the waveguide 125 may be of course varied. The chill blocks 122 may be constructed of many suitable heat transfer materials, and are preferably formed of materials with high thermal conductivity such as copper, aluminum, sapphire, or synthetic diamond.

The heat that is transferred to the cooling blocks 122 may then be removed from the cooling blocks using any number of other conventional heat removal techniques, such as flowing a coolant fluid through the chill blocks or contacting the chill blocks to a thermal electric cooler. The thermal management system 120 shown in Fig. 12 may operate with an optically pumped waveguide laser. The laser may include a pair of reflective mirrors monolithically, or non-monolithically (not shown), formed with a planar waveguide to define an optical cavity with an optical axis. A reflective mirror may be mounted relatively external to the gain medium or monolithically formed with the waveguide. The planar waveguide 125 may be centrally disposed along the optical axis of the waveguide having a plurality of side surfaces. The waveguide 125 may include a gain medium layer 129 formed with an upper surface and a lower surface, and may be capable of sustaining a population inversion. In addition, the inner surfaces of a pair of cladding layers 127 may be respectively bonded to the upper and the lower surface of the gain medium layer 129. The interface formed between each inner surface of the cladding layers 127 and the gain medium layer 129 define a first waveguide section for spontaneous emission of the medium by virtue of an index of refraction discontinuity. Transverse mode discrimination may be accomplished substantially by differential resonator mode losses. In addition, the transverse mode discrimination in the unguided direction may be accomplished through differential resonator mode losses, and/or mode discrimination in the guided direction may be accomplished through the first waveguide. The outer surfaces of the cladding layers 127 define a second waveguide section by virtue of an index of refraction discontinuity for containing pump radiation within the waveguide from an optical pump source. In addition, a first and a second external layer 123 formed of a laser-inactive medium may be respectively

positioned substantially adjacent to the outer surface of each cladding layer 127.

The interface formed between each outer surface of the cladding layers 127 and each external layer 123 may also define a waveguide section for confinement of pump radiation by virtue of another index of refraction discontinuity. An optical pump source (not shown) may provide pump radiation to the waveguide across at least one side surface of the planar waveguide along the direction of or perpendicular to the optical axis, or along any other direction with respect to the optical axis of the waveguide. The optical pump source may include at least one laser diode, and may be positioned relatively parallel or perpendicular to the optical axis. Pump radiation may be of course injected into the pump region from a variety of other directions relative to the optical axis of the waveguide, and may also provide radiation across a side surface of the planar waveguide that is relatively parallel or perpendicular to the optical axis. As with other described embodiments, external cylindrical lenses or other intermediary optics may be positioned between the optical pump source and the planar waveguide.

A variety of suitable reflective and anti-reflective optical coatings may be also applied or included along selected surfaces of the planar waveguide.

Additionally, the optically pumped waveguide may further include a medium capable of acting as a saturable absorber/passive q-switch.

Another embodiment of a waveguide cooling system 130 is shown in Fig. 13 in which only one chill bar or block 132 is in thermal contact with a waveguide 135 surface. This variation of selected cooling architecture may be preferable for particular applications including laser systems where it may be advantageous to leave a planar surface of the waveguide exposed to ambient surroundings. The heat transfer achieved by cooling only one surface of the waveguide 135 may sufficiently remove waste heat generated by the structure.

The addition of another top capping block or cooling body may be of course included in addition.

Fig. 14 illustrates yet another variation of a compound waveguide geometry provided in accordance with the invention. The top layer of the waveguide 145 may be omitted, and the pump radiation may still remain

confined to the top three layers, namely the laserable core 149 and two adjacent cladding layers 147. Cooling of the waveguide 145 may be accomplished by a chill bar (not shown) through a lower external layer 143 or bottom surface of the structure as shown in Fig 13. The top surface 141 of the waveguide 145, or the external surface of the top cladding layer 147, may be simply left exposed to the ambient surroundings. Even without a top external layer, the pump radiation may be confined by the interface between the external layer 143 and the ambient surroundings. The developed laser radiation may be confined to the laserable core 149 by its interface with each cladding layer 147.

Another configuration for the waveguide systems described herein may be derived by taking the limiting case in which the thickness of the inner pump cladding layers shrinks or goes to zero. This is a degenerate case in which the developed laser radiation and the pump excitation radiation essentially become confined by the same waveguide structure 155. As shown in Figs. 15-16, the regions forming the pump radiation waveguide and the waveguide that confines the generate laser radiation may essentially converge. As the thickness of the inner or intermediate pump cladding layer 157 approaches zero, the outer pump cladding layers 153 becomes in essence a waveguide section 159 that now serves to confine both the pump and the developed laser radiation. Fig. 16 is another variation of this architecture in which the top outer cladding layer is also omitted. The pump radiation and the developed laser radiation in this configuration may be confined to the top single laserable layer or core 169, and cooling of the waveguide 165 may be also performed with a chill bar or cooling element (not shown) through the lower outer cladding layer 167 and the bottom layer 163 of the waveguide, while the top surface of the core is simply left exposed to the ambient surroundings. The core and cladding compound waveguides described herein may thus provide independent confinement structures for pump radiation and developed laser radiation with numerous layers of either 2,3,4 or 5 layers or more in total as described in the above figures.

Another aspect of the present invention may be directed to solid state laser (SSL) systems for generating linearly polarized output. The ability of applied stress to alter the polarization properties of isotropic crystals is generally known for rod lasers. For example, unstressed laser rods fabricated from isotropic laser crystals do not generally exhibit preferred eigenpolarization directions. However, these rods under a thermal load apparently show a dramatic change. Under uniform thermal loading, the preferred eigenpolarization directions become well defined and are coincident with the local radial and tangential directions as defined by the axis of a laser rod. These local radial and tangential eigenpolarization directions are coincident with the principal directions of the local optical indicatrix, which becomes perturbed from its originally spherically symmetric shape due to the photoelastic effect which often couples the thermally induced stress tensor to the optical indicatrix.

Thus, under typical operating conditions the output from such thermally loaded laser rods would be unpolarized because different locations in the rod would lase with different preferred polarization directions. Furthermore, such laser rods often act to depolarize existing polarized radiation that is transmitted through them.

In order to achieve lasing in a specific polarization with such laser rods, which are fabricated from isotropic crystalline or glass material, polarization selective components are often placed within the laser cavity. This results in a polarization direction to see a large loss and so as to be effectively suppressed.

The drawback of this technique often is that because the laser rod acts to depolarize already polarized laser radiation, the polarization selective component introduces a loss each round trip through the laser cavity by sweeping out the laser radiation with the undesired polarization. This incurred loss in every round trip may seriously limits the efficiency and output power possible. On the other hand, if the laser rod provided well-defined eigenpolarization directions, a polarizer placed in the cavity aligned with one of these eigenpolarization directions would in principle introduce no loss as the laser rod would not depolarize the laser radiation on every round trip. The

elimination of polarization selective components within the cavity would thus provide more efficient laser operation.

By using dissimilar materials to form compound laser components with differing coefficients of thermal expansion bonded together at elevated temperature in accordance with the present invention, it is possible to engineer in stresses that may be permanently present when the composite sample temperature is returned to its normal operational temperature. By engineering these stresses to be substantially larger than the thermally induced stresses that will be encountered in the structure under laser operation conditions, it is then possible to design structures that will be relatively insensitive to the stress induced by the thermal loading. This generally follows if the thermal stresses substantially appear as small perturbations to the larger stresses that were engineered in during the sample fabrication. In effect, this is the same principle by which thermal stresses do not impact the polarization properties of naturally birefringent crystals such as YLF. In such anisotropic crystals, thermal stresses are present and couple to the optical indicatrix through the elasto-optic effect, but in practice, the resulting change to the optical indicatrix is in general so minor as to be relatively unimportant to normal laser operation.

Another embodiment of the invention includes the design of surface figures with materials that are bonded such that the components deform during optical contact between two surfaces to be bonded. A permanent stress is thus created between the two parts that is not annealed out during subsequent heat treatment. A generally operable and preferable method of creating mechanical stress birefringence includes forming a compound structure between the isotropic lasing medium, either crystalline or vitreous, and at least one or preferably two layers of a non-lasing material. A preferable method again is to form an adhesive-free bond between the lasing and non-lasing material by optical contacting and subsequent heat treatment. In general, however, any technique of bonding materials that have, or develop during laser operation, stress birefringence simulating anisotropy of a birefringent crystal, may be

operational in accordance with the invention wherein the stressing condition is stable and the lasing operation desirable.

Accordingly, by choosing a material combination of laser medium and mechanical stress-inducing material that is stable under the exerted stress and during laser operation, the desired mechanical stress condition may be achieved by heat treating optically contacted materials with a difference in coefficients of thermal expansion (CTE). Differences in thermal expansion exist for many lasing and non-lasing materials. However, the choices are often narrowed by other conditions such as compatibility in a compound structure and stability during lasing operation. Stress inducing materials may be crystalline or vitreous. Differences in thermal expansion coefficients may be relatively small in the order of about 5 x 10-'/°C or larger. All of these combinations may be operable because process variations such as heat treatment times, heat treatment temperatures, bonding process conditions in general, aspect ratios and compound configurations, may all have an influence that can lead to the desired linearly polarized output. By way of example, a preferable embodiment of the present invention allows a choice between a compound formed between two or more materials with a large difference in CTE and a low temperature heat treatment, or a compound formed between materials of a small CTE and an accordingly higher temperature heat treatment. In a practical situation, other considerations such as mechanical strength, stability during laser operation, thermal conductivity and refractive index may narrow the available materials combinations for compound formation.

The chemical reactivity of the components making up the composite structures described herein has a strong effect on the stress that is retained after heat treatment as a function of temperature. When the reactivity between components is low at heat treatment temperatures, it has been observed that the bonded components slide with respect to each other to significantly eliminate stress. As a result, a composite structure is provided that will have minimal or hardly any residual stress in the bulk of the lasing medium. As explained above, this will therefore not give rise to linearly polarized output of laser radiation in

general. On the other hand, if the heat treatment temperature is high enough to cause a chemical reaction at the interface of two dissimilar materials, then the components generally adhere to each other at the heat treatment temperature, and sliding to prevent stress is prevented. Under these conditions, a pre-stressed lasing component will result that can lase with linearly polarized output as long as that stress is higher than that generated by the temperature rise during lasing operation.

It has been further observed that the bond strength does not generally depend on the chemical reactivity of the components with each other. It is assumed that this chemical reactivity also depends on the crystallographic orientation of crystals with respect to each other. While temperatures for chemical reaction between components at their interface often depend on the nature of the individual components, specifically tested examples illustrate this general behavior. For example, it has been observed that heat treatment of YAG/sapphire compound structures result in negligible stress in the bulk of the YAG at temperatures below about 1200 C. At a heat treatment temperature of 1375 C for 4 hours, it has been observed there is substantial stress retained in the lasing medium that causes linearly polarized laser output. Moreover, the adhesion of YAG and sapphire components to each other has been observed by a change in the interference fringe pattern from originally uniform fringes to fringes that at the YAG/sapphire interface after heat treatment to 1375 C exhibit a waviness at the interface due to the relative shift of components to each other that is not reversible. In addition, a sliding is observed between YAG and sapphire to equalize or offset stress build-up. The YAG and sapphire constituents slide with respect to each other to essentially eliminate stress build- up. A variety of interferometric techniques evidence this relative movement between the YAG and sapphire. When there is a chemical reaction such as this 1375 C heat treatment provided in accordance with the invention, the specific effect that results is YAG acting as a non-isotropic material. It should be recognized however that heat treatment to temperatures beyond about 1400 C would not generally result in a substantial increase in stress because sapphire

would plastically deform to counteract further stress as the temperature increases. The desired effects described herein may be also applicable for sapphire and other crystal or glass materials that are non-reactive up to selected temperatures, and may be further applicable beyond sapphire to materials before and after they are chemically reactive at the interface.

In accordance with this aspect of the invention, a preferable combination of lasing crystal and stress inducing material provides a lasing medium of the garnet crystalline structure bonded into a compound structure with sapphire that is arranged parallel to the direction of laser proportion. Among the most frequently used lasing materials are trivalent rare earth ions of Nd, Tm, Ho, Er and Yb doped into a non-lasing talline lattice. One of the most frequently used isotropic lasing material is Nd: YAG, while one of the nonlasing materials of most versatile properties in a lasing environment is sapphire in terms of mechanical strength, thermal conductivity and chemical inertness. In accordance witt the invention, a Nd: YAG-sapphire compound configuration may be selected with an actual lasing architecture that is chosen by laser performance considerations. However, stress imparted by the sapphire to the lasing medium by means of bonded compound formation should be generally larger than the thermal stress birefringence due to laser operation as described above. The following examples serve to further demonstrate the advantages of the present invention with Nd: YAG/sapphire compounds with different SSL system architectures.

EXAMPLE 1-A waveguide laser with a Nd: YAG core and linearly polarized output.

A waveguide laser design provided in accordance with the invention is shown in Fig. 17. The Nd: YAG core is approximately 20 microns thick, and the udoped YAG pump cladding layers directly adjacent to the core are approximately 5 microns thick. The sapphire outer cladding layers 170, which are bonded at high temperature to the YAG, introduces a permanent stress in the central YAG layers 172 to generate eigenpolarization directions that are parallel to and perpendicular to the bond plane. The illustrated device generates

diffraction limited radiation in the guiding dimension (the vertical dimension in the diagram) by strongly favoring the desired high beam quality fundamental mode over other higher order transverse modes. This process which is generally known as mode matching may be accomplished in the device by taking advantage of the fact that the fundamental mode is strongly concentrated near the center of the three guiding layers (the YAG/Nd: YAG/ YAG layers) while the next higher order modes tend to have more of their fields in those portions of the three layers near the outer edges of the layers. Accordingly, the fundamental mode's field is preferentially centered on the central Nd: YAG gain loaded core 174 of the device, and thus sees a higher gain than the next higher and undesired transverse modes. This higher gain, which is seen by the fundamental mode, allows this mode to reach threshold first and lase preferentially before other modes have a chance to build up.

As shown in Fig. 18, the mode fields calculated for this device as shown illustrate the manner in which the fundamental mode is concentrated near the center of the guiding layers more strongly than the next higher mode. Fig. 18 illustrates the calculated mode intensity for the fundamental and the first mode shown from the centerline of the waveguide out towards the sapphire outer cladding layer. So in this plot, the region from 0 to 10 microns corresponds to half the doped core layer, with 0 being at the waveguide's center. The region from 10 microns to 15 microns corresponds to the undoped YAG pump cladding layer, and the region beyond 15 microns corresponds to the outer sapphire layer. The plot above is symmetric around the origin, but the bottom half of the waveguide is not shown. A first line 180 is the profile of the desired fundamental mode and is peaked at the center of the waveguide. A second line 182 is the next higher transverse mode and has a null at the center of the waveguide and peaks somewhat away from the waveguides center. The parameters listed in the table below correspond to those used in deriving the field intensities in the above plot and are explained further with the help of the diagram following the table below. 1.064 Wo vacuum wavelength of laser light (microns) YAG layer refractive index 1.8296 n2 Intermediate layers (undoped YAG) refractive index 1.76 n3 outer layers (sapphire) refractive index 20 t, central layer thickness (microns) 5 t2 intermediate layer thickness (microns)

To calculate the effectiveness of the mode matching discrimination, which strongly favors the fundamental mode, the mode overlap values, which give that fraction of the mode's energy that resides in the gain loaded core layer, can be calculated once the mode fields are derived. For the case under consideration here, the mode overlap values of the fundamental and next higher transverse mode are calculated to be 0.94 for the fundamental vs. 0.80 for the next higher mode. For the Nd waveguide above, this level of discrimination ensures single transverse fundamental mode operation.

The mode fields shown above are calculated straight forwardly by finding the electric field solutions that satisfy, which describes the transverse electric field envelope in the waveguide. In the above equation, x is the transverse coordinate, n is the refractive index which varies from layer to layer, and P is the mode propagation constant which characterizes the various modes possible in the waveguide structure.

As previously described herein, five-layer waveguide structures may be constructed using pump cladding regions that have indices of refraction that are smaller than the doped core region. A sapphire/YAG/Nd: YAG/ YAG/sapphire five layer waveguide is a previously described example with a central doped Nd: YAG layer having a slightly higher index than the undoped YAG layers due to the polarizability of the Nd dopant in the central layer. However, the use of cladding layers having a refractive index lower than or equal to that of the

central doped layer is not absolutely essential for fundamental mode operation.

This is at least partially due to the observation that the modal properties of this class of waveguide devices is governed by mode overlap considerations with the gain core in addition to the guiding properties of the waveguide structure itself.

In fact, it is possible to engineer fundamental modes that have more of a top hat characteristic than was the case in the previously discussed Nd: YAG waveguide structure. Instead of having the cladding layer of a slightly lower refractive index, its is possible using cladding layers on each side of the central doped layer that have slightly higher index than the central doped layer. 1.064 ko vacuum waveiength of laser light (microns) YAG layer refractive index 1.8315 n2 Intermediate cladding layer refractive index 1.76outer layers (Sapphire) refractive index 20 t, central layer thickness (microns) ~ t2 intermediate thickness (microns) For example, Fig. 19 illustrates the mode intensity of the fundamental and first mode when the refractive index of the inner cladding layer is larger than that of the core. The dimensions of all the layers may remain the same as the previously discussed Nd: YAG waveguide, and only the refractive index of the intermediate guiding layers may be changed. In this case, the fundamental mode is still preferred over the next higher transverse mode due to its improved mode matching to the central gain core of the device. The mode overlap values of the fundamental and next higher transverse mode are calculated to be 0.82 for the fundamental vs. 0.62 for the next higher mode. In general, the effect of the higher index in the pump-cladding region is to pull more of the mode's energy into that region and away from the central doped core region of the waveguide.

In circumstances where the near field mode intensity is desired to be more uniform than say a typical gaussian fundamental mode, the ability to engineer mode profiles through proper refractive index selection is an important capability of the present invention. Such top hat-profiles will for example have certain advantages when used for frequency conversion in nonlinear crystals.

The waveguide devices herein may incorporate the use of canted sides to assist in the suppression of unwanted parasitic lasing modes. Parasitic lasing modes are undesirable as they can rob gain from a preferred laser mode. One example of these parasitic lasing modes is illustrated in Fig. 20 which shows a top view of a waveguide. In this diagram, a ray of light can be trapped within the waveguide for very long path lengths due to total internal reflection at the sides of the guide. Looking down on the waveguide from above, there are many closed paths that are totally confined by total internal reflection at the YAG to air interfaces (the critical angle at these interfaces is-33.5 degrees).

Given sufficient gain in the waveguide, such trapped rays can effectively extract much of the stored energy in the waveguide therefore making it unavailable to the desired laser mode, and so negatively impacting the laser's performance.

One way to frustrate the internal parasitic ray paths shown in the above diagram is by canting the sides of the waveguide as shown above. In the case of a waveguide with canted sides, rays that may begin as a trapped ray will have an angular displacement imparted to its propagation direction every time it reflects off a canted side. Importantly, these angular displacements will tend to want to throw the parasitic ray out of the guiding region of the waveguide because of its limited numerical aperture. Once a ray can begin to leak out of the guiding layers of the waveguide it will see higher losses, and if these losses are higher than the gains seen by the ray in the waveguide, then the ray's effectiveness for depleting stored gain will have been neutralized or significantly reduced. In practice, it has been observed through experimentation, cant angles on the sides of the guide as small as 1 degree can be effective at reducing the deleterious effects of these trapped parasitic rays. The technique used here to suppress parasitic rays is broadly applicable to all the waveguide devices being described within.

This technique of controlling parasitics is generally applicable to waveguide lasers, even when they are configured as unstable resonators, or consist of more complicated core structures as described herein.

EXAMPLE 2-Waveguide laser with Yb: YAG core and linearly polarized output Fig. 21 shows that the waveguide laser architecture may consist of a core layer 210 of Yb: YAG with undoped YAG ends 212 on both sides, outer cladding layers 214 but without undoped cladding layers. Canted sides may again prevent or reduce parasitic oscillations to reduce the available gain for laser operation. As noted above with Example 1, the waveguide laser exhibits linearly polarized output. A wide variety of waveguide laser designs is accessible to this invention, including passively q-switched lasers and unstable resonator designs, and a range of 4f transition metal dopant ions in YAG, other garnet structures or in other isotropic media. It should be noted these and many other aspects of the present invention described herein are not restricted to waveguide lasers. It has been observed between crossed polarizing films or prisms that mechanical stress birefringence can be induced in other, more common configurations that are of use in solid state lasers. The following examples schematically illustrate a selection of configurations of laser rods, laser slabs, microchip lasers and fiber lasers that lase with linearly polarized output.

EXAMPLE 3-Compound Nd: YAG/sapphire rod Fig. 22A depicts a compound Nd: YAG rod that consists of a near- cylindrical Nd: YAG component 220 with two sapphire components 222 adhesive-free bonded to it. Induced stress birefringence may be observed between crossed polarizing films, resulting in linearly polarized laser radiation when inserted into a laser cavity and pumped with laser diode bars.

Fig. 22B illustrates an arrangement of a compound Tm: YAG laser rod with essentially elliptical cross section, consisting of a Tm: YAG section 224 to which two undoped YAG ends 226 are adhesive-free bonded. This compound of Tm: YAG and undoped YAG has two outer cladding layers of sapphire 228 bonded to it that impart the mechanically induced stress to the central YAG compound. The lens-like sapphire layers also may be employed to introduce pump radiation from laser diode bars to the laser rod. In addition, the near-

elliptical cross section of the compound rod provides the advantage of eliminating parasitic oscillations, known as whispering gallery modes, that propagate along the circumference of laser rods with circular cross-sections.

Fig. 22C demonstrates another example within the wide range of useful laser rod architectures that can be engineered to emit linearly polarized laser output in accordance with the invention. A generally tapered 229 rod may include a compound core of undoped YAG 221/doped Yb: YAG 223 has two undoped YAG sides 225 and two sapphire layers 227 bonded to it, resulting in a birefringent YAG section of the rod.

EXAMPLE 4-Nd: YAG/sapphire slab Figs. 23A-B demonstrate schematically the applicability of the present invention to compound laser slab configurations as another commonly employed geometry of solid state lasers. Fig. 23A illustrates a compound zig- zag slab lasing with linearly polarized output. It consists of a central compound Yb: YAG component 230, with two undoped YAG ends 232 that are adhesive- free attached to it with techniques described herein. The YAG compound in turn is sandwiched between two sapphire sides 234 that cause the YAG to behave as a quasi-birefringent material. Fig. 23B is a similar zig-zag slab with Brewster angles, except that Nd: YAG 236 is the laserable material that develops stress birefringence due to two sapphire layers 238 that are bonded to it as shown.

EXAMPLE 5-Nd: YAG/Cr4: YAG microchip Fig. 24A shows a high-power passively q-switched compound Yb: YAG microchip laser consisting of undoped YAG ends 240, Yb: YAG as lasing crystal 242, Cr4+: YAG 244 as saturable absorber, and sapphire sides 244. The propagation of the direction of the laser beam 245 is parallel to the sapphire cladding layers. Fig. 24B shows a simplified version, for relatively lower output power, where the lasing element Nd: YAG 246 is compounded with Cr4+ : YAG 248 as saturable absorber for passively q-switched operation. Sapphire sides 244 provide the stress birefringence in the YAG compound structure for linearly polarized laser output.

Fig. 25 illustrates a specific example of a preform provided in accordance with yet another aspect of the present invention. A core of square cross-section of laserable phosphate glass 250 of refractive index n, is adhesive- free bonded on two of its sides with a laser-inactive glass 252 of essentially same coefficient of thermal expansion a,, and refractive index n2, where n, >n2.

The remaining two sides of the compound preform are formed from a phosphate glass 254 of a lower coefficient of thermal expansion a2, and refractive index n2.

The length of the preform can vary be between approximately 2-20". The viscosity versus temperature curve of the component glasses of the preform should be compatible with redrawing, and is desirably similar for all components. One-step redrawing to reduce the dimensions of the cross section of the preform to 1/5 to 1/15 of its original size is available in the prior art. A second redrawing process may follow to further reduce the cross section if desirable. The lower expansion coefficient of the two outer layers 254 imparts a mechanical stress birefringence onto the laserable core that results in lasing with linear polarized output. A number of variations of these embodiments are conceivable and commercially useful. Similarly to the discussion on waveguides above, mode overlap may be employed to engineer the beam shape and quality of the output laser. A double-clad architecture with an outer cladding layer of refractive index n3 gives results that are equivalent to those discussed under crystal waveguides. Refractive index nl may be either larger, same or smaller than n3, resulting in different mode overlap effects. It shall be understood that these preceding six examples are representative of the present invention. Many other combination of materials may be provided herein that result in the benefits of the present invention.

While all aspects of the present invention have been described with reference to the aforementioned applications, this description of various embodiments and methods shall not be construed in a limiting sense. The aforementioned is presented for purposes of illustration and description. It shall be understood that all aspects of the invention are not limited to the specific materials, parameters, depictions, configurations or relative proportions set forth herein. The specification is not intended to be exhaustive or to limit the invention to the precise forms disclosed herein. For example, the intermediate coupling optics that may be used to deliver the pump radiation into the waveguide structure may be more elaborate than the relatively simplified cylindrical lens shown, and in particular, may consist of several lensing or other optical elements. Furthermore, where single diode array bars are shown, multiple diode array bars may be positioned in a stacked configuration with the coupling optics consisting of multiple lensing elements and/or a lensing duct.

Other various modifications and insubstantial changes in form and detail of the particular embodiments of the disclosed invention, as well as other variations of the invention, will be apparent to a person skilled in the art upon reference to the present disclosure. It is therefore contemplated that the appended claims shall cover any such modifications or variations of the described embodiments as falling within the true spirit and scope of the invention.