Low-cost and compact blue/green lasers are desired for applications such as micromachining, laser display, underwater communications, high-density optical data storage, and medical diagnostics recently. Therefore various type of blue and green lasers have been studied, especially for intracavity frequency doubling of the diode-pumped solid-state laser, which can generate high blue/green powers with long lifetime. Unlike the green laser, which is originated from a four-level laser, the blue laser belongs to a quasi-three-level system, so it is more difficult to develop the blue laser source. The purpose of this experiment is to develop a high power and high efficiency blue laser with simple structure so that it can easily be commercialized. Furthermore, it is a very cost-effective approach to develop such solid-state lasers, if the laser output characteristics can be estimated precisely using software simulation. We used an optics software GLAD to model our four-level and quasi-three-level Nd:YAG laser systems. In experiment, we developed a blue laser system with a cavity length of 4 mm and with 71.7 mW of blue output power. Besides, we have succeeded in using GLAD to model a Nd:YAG plane-parallel laser cavity, which has an optical conversion efficiency of 68%. Finally, we designed an effective lens duct with a coupling efficiency up to 80%, even if there is no AR coating on lens duct¡¦s input or output facets.

Abstract As blue/green laser has a short wavelength radiation, it can be applied to micro-machining, laser display, high-density optical data storage, underwater communications, and so on. Large efforts have been devoted to simplify the laser system and reduce the cost. Therefore, various types of blue/green lasers have been studied, especially intracavity frequency doubling of the diode-pumped solid-state laser, which can effectively generate high blue/green laser powers with long lifetime. Among all cavity designs, direct-coated composite crystal is the most compact structure. Compare with the green laser, which is a four-level laser, blue laser belongs to a quasi-three-level system. Thus, it is more important to control the temperature of gain medium. Before the experiment, making an estimation will greatly benefit the progress and efficiency. ZEMAX was utilized to simulate the focus system and GLAD was used to model our intracavity frequency-doubled blue laser. In the experiment, we used a LD array as a pumping source and arranged suitable lens to reduce the array¡¦s spot size. The laser crystal was mounted onto a copper mount which was cooled by the Vapochill cooling system. In addition, we also tried to rotate the crystal and obtained a peak power of 192 mW with only 4 mm cavity length. The result is the highest output power of microchip blue laser to our knowledge. Using lens duct as the pump transport optics can further miniaturize this composite-chip blue laser.

The purpose of this thesis is to develop a high power, compact all solid-state blue laser, which is applicable in micro machining, LIDA, underwater ranging, biochemical techniques and so forth. The passive Q-switching technique, which is known to be a low-cost and simple method to raise the laser peak power was employed in this thesis. In the mean time, the intracavity-doubling technique was integrated to achieve the non-linear frequency conversion for generating blue laser at low cost. Based on our research finding, the reabsorption loss due to thermal effect and a paucity of suppression at wavelength of 1064 nm on laser mirrors could cause the four-level oscillation at 1064 nm instead of three-level oscillation at 914nm. Improvement in heat dissipating system, and suppression at wavelength of 1064 nm on mirror coating has led to a success in developing a quasi-three-level blue laser with peak power of 114W at wavelength 473 nm. A modified rate equation model of the quasi-three level passively Q-switched blue lasers was developed as well, in which the influence of the re-absorption loss in the gain medium and its intracavity frequency doubling were both considered. The influence of reabsorption loss upon the laser power deduction was studied by numerical simulation in order to optimize the laser performance.

Because compact solid-state blue/green lasers can generate high power, and short wavelength radiation, it is applied in micromaching, laser display, underwater ranging, and so forth. It is a very cost-effective approach to develop such lasers, if the laser output characteristics can be estimated precisely using software simulation. The purpose of this study is to use an optics software GLAD (General Laser Analysis and Design) to model our intracavity frequency-doubled blue/green lasers. The GLAD software considers the wave nature of laser, such as dispersion and diffraction. Moreover, it employs a modular design in modeling linear or nonlinear optical components. In order to get more precised estimation of the laser output characteristics of a quasi-three-level laser, the laser model in GLAD was modified to take into account the reabsorption loss in gain medium. In our experiment, blue/green microchip lasers were developed. We used a 3W LD to pump a quasi-three-level laser with the Nd:YAG crystal as gain medium and KNbO3 crystal as the intracavity SHG crystal for the generation of blue laser. The laser generates 17.6 mW of blue power with a cavity length of 4 mm. With almost the same structure except using Nd:YVO4 crystal as gain medium and KTP crystal as the intracavity SHG crystal for generation of green laser, the laser produces 627 mW of green power with a cavity length of 6 mm.

No description available.

The purpose of this study is to develop a solid-state blue laser which has advantages of high power, short wavelength, and compact. It can be applied in micromaching, LIDAR, underwater ranging, biochemical techniques, and so forth. We increased the peak power of the laser effectively by a low-cost, small, and easy-use passive Q-switching technique. In addition, intracavity frequency-doubling is an economic way to achieve non-linear frequency conversion for blue generation. By integrating of these two techniques, we develop a compact all solid-state high-power blue laser with 83 W peak power at 473 nm. Restricted to reabsorption loss, the optical to optical conversion efficiency of 4F3/2 ¡÷ 4I9/2 quasi-three-level laser is lower than 4F3/2 ¡÷ 4I11/2 four-level laser for Nd:YAG crystal. The reabsorption loss will change with the temperature variation of the gain medium, it enormously affects to the performance and stability of quasi-three-level lasers. Therefore, in addition to make systematic studies of the conversion efficiency of KNbO3, BBO, LBO as the intracavity SHG crystals for generation of high-power blue laser, we use the numerical analysis to investigate the influence of reabsorption loss to quasi-three-level passive Q-switching laser. At present, blue laser with peak power of 83 W and pulse width of 10.6 ns was generated as a result. To our knowledge, the compact all solid-state high-power pulsed blue laser is demonstrated for the first time by integrating of passive Q-switching and intracavity frequency-doubling simultaneously.

Lasers operando nas regiões espectrais do azul e do amarelo-laranja foram recentemente requisitados pelo mercado de aplicações quer para melhorar as tecnologias já conhecidas ou para possibilitar a criação de novas. Isso é devido às propriedades destas regiões espectrais, com o azul trazendo características tais como fótons de alta energia e feixes limitados por difração menores, enquanto a faixa do amarelo-laranja é ainda uma região espectral difícil de se atingir e não foi totalmente acessada ou nem mesmo acessada por fontes de luz laser eficientes. Aplicações dos lasers azuis são encontradas em tecnologias de alta densidade de armazenamento, displays a laser, sistemas LIDAR, pinças ópticas e uma longa série de aplicações que exigem alta precisão. Os lasers amarelo-laranja também têm aplicações importantes, destacando-se aplicações em cirurgia oftalmológica a laser, em displays de cores reais e como estrela guia (excitando linhas de sódio na atmosfera). A investigação de lasers de quase três níveis e laser Raman de Nd:YLF foi realizada neste trabalho. A finalidade é de propor fontes laser de alta potência e eficientes emitindo no azul e no amarelo para suprir as aplicações. Eficiência e potências de saída da ordem de Watt foram demonstradas para um laser de Nd:YLF emitindo em 908 nm assim como no segundo harmônico em 454 nm. Além disso, lasers Raman de Nd:YLF/BaWO4 e Nd:YLF/KGW foram demonstrados atingindo alguns Watts de potência de saída em regime quasi-CW e CW, com boas qualidades de feixe (M2 2) e em oito comprimentos de onda diferentes: 1147 nm, 1163 nm, 1167 nm , 549 nm, 552 nm, 573 nm, 581 nm e nm 583. Por fim, uma luminescência azul originada em alguns cristais Raman, durante a oscilação Stokes, teve sua origem e seus efeitos colaterais para lasers (perdas e calor adicionais) minuciosamente caracterizados. / Lasers operating in the blue and yellow-orange spectral regions are sought after by the applications market either to improve well known technologies or to enable new ones. Blue lasers bring features such as high energy photons and smaller diffraction limited beams, while the yellow-orange range is a hard to reach spectral region where there is a considerable shortage of efficient laser light sources. Applications of the blue lasers are found in high density storage technologies, laser displays, LIDAR systems, optical tweezers and a long range of high precision demanding applications. The yellow-orange lasers also have important applications, with highlights in ophthalmologic laser surgery (photocoagulation), in true color displays and as a guide star (exciting sodium lines in the atmosphere). The investigation of Nd:YLF quasi-three level lasers and Nd:YLF Raman lasers was further studied in this work in order to provide high power and efficient blue and yellow lasers sources. Demonstrations of efficient and multi-Watt operation of a 908 nm laser and its respective second harmonic laser at 454 nm are described. Also, Nd:YLF/BaWO4 and Nd:YLF/KGW Raman lasers were demonstrated reaching Watt levels in quasi-CW and CW regime with very good beam qualities (M2 2) at eight different wavelengths: 1147 nm, 1163 nm, 1167 nm, 549 nm, 552 nm, 573 nm, 581 nm and 583 nm. Finally, a blue luminescence originating in some Raman crystals, during Stokes oscillation, has been studied in considerable detail. Its origin and consequences for laser operation (extra loss and heat load) have been identified.

Lasers operando nas regiões espectrais do azul e do amarelo-laranja foram recentemente requisitados pelo mercado de aplicações quer para melhorar as tecnologias já conhecidas ou para possibilitar a criação de novas. Isso é devido às propriedades destas regiões espectrais, com o azul trazendo características tais como fótons de alta energia e feixes limitados por difração menores, enquanto a faixa do amarelo-laranja é ainda uma região espectral difícil de se atingir e não foi totalmente acessada ou nem mesmo acessada por fontes de luz laser eficientes. Aplicações dos lasers azuis são encontradas em tecnologias de alta densidade de armazenamento, displays a laser, sistemas LIDAR, pinças ópticas e uma longa série de aplicações que exigem alta precisão. Os lasers amarelo-laranja também têm aplicações importantes, destacando-se aplicações em cirurgia oftalmológica a laser, em displays de cores reais e como estrela guia (excitando linhas de sódio na atmosfera). A investigação de lasers de quase três níveis e laser Raman de Nd:YLF foi realizada neste trabalho. A finalidade é de propor fontes laser de alta potência e eficientes emitindo no azul e no amarelo para suprir as aplicações. Eficiência e potências de saída da ordem de Watt foram demonstradas para um laser de Nd:YLF emitindo em 908 nm assim como no segundo harmônico em 454 nm. Além disso, lasers Raman de Nd:YLF/BaWO4 e Nd:YLF/KGW foram demonstrados atingindo alguns Watts de potência de saída em regime quasi-CW e CW, com boas qualidades de feixe (M2 2) e em oito comprimentos de onda diferentes: 1147 nm, 1163 nm, 1167 nm , 549 nm, 552 nm, 573 nm, 581 nm e nm 583. Por fim, uma luminescência azul originada em alguns cristais Raman, durante a oscilação Stokes, teve sua origem e seus efeitos colaterais para lasers (perdas e calor adicionais) minuciosamente caracterizados. / Lasers operating in the blue and yellow-orange spectral regions are sought after by the applications market either to improve well known technologies or to enable new ones. Blue lasers bring features such as high energy photons and smaller diffraction limited beams, while the yellow-orange range is a hard to reach spectral region where there is a considerable shortage of efficient laser light sources. Applications of the blue lasers are found in high density storage technologies, laser displays, LIDAR systems, optical tweezers and a long range of high precision demanding applications. The yellow-orange lasers also have important applications, with highlights in ophthalmologic laser surgery (photocoagulation), in true color displays and as a guide star (exciting sodium lines in the atmosphere). The investigation of Nd:YLF quasi-three level lasers and Nd:YLF Raman lasers was further studied in this work in order to provide high power and efficient blue and yellow lasers sources. Demonstrations of efficient and multi-Watt operation of a 908 nm laser and its respective second harmonic laser at 454 nm are described. Also, Nd:YLF/BaWO4 and Nd:YLF/KGW Raman lasers were demonstrated reaching Watt levels in quasi-CW and CW regime with very good beam qualities (M2 2) at eight different wavelengths: 1147 nm, 1163 nm, 1167 nm, 549 nm, 552 nm, 573 nm, 581 nm and 583 nm. Finally, a blue luminescence originating in some Raman crystals, during Stokes oscillation, has been studied in considerable detail. Its origin and consequences for laser operation (extra loss and heat load) have been identified.

A near-field technique known as evanescent interferometric lithography allows for high resolution imaging. However its primary limitation is that the image exponentially decays within the photoresist due to physical limits. This thesis aims to overcome this limitation and presents a method to considerably enhance the depth of focus of images created using evanescent interferometric lithography by using a material underlay beneath the photoresist. A key enabler of this is the understanding that evanescent fields couple to surface states and operating within proximity of a resonance, the strength of the coupling allows for considerable energy extraction from the incident beam and redistribution of this energy in a photoresist cavity. This led to the analysis of the Fresnel equations, which suggested that such coupling was in fact the result of an enhanced reflectance that takes place at boundaries of carefully chosen materials. While it is known that metals and lossy dielectrics result in surface plasmon polaritons (SPP) and surface exciton polaritons (SEP) as conventional solutions to the Fresnel reflection equations for the TM polarization of light, there is no such naturally occurring surface state that allows evanescent wave enhancement with the TE polarization of light. Further investigation of the Fresnel reflection equations revealed both for TM and TE that in fact another solution exists that is but unconventional to enhance the reflectivity. This solution requires that one of the media have a negative loss. This is a new type of surface resonance that requires that one of the media be a gain medium; not one in the optical pumped sense but one that would naturally supply energy to a wave to make it grow. This new surface resonance is also a key result of this thesis. Clearly, however this is only a hypothetical solution as a real gain medium would violate the conservation of energy. However, as it is only the reflectance of this gain medium that is useful for evanescent wave enhancement, in fact a multilayered stack consisting of naturally occurring materials is one way to achieve the desired reflectivity. This would of course be only an emulation of the reflectivity aspect of the gain medium. This multilayered stack is then an effective gain medium for the reflectivity purposes when imaging is carried out at a particular NA at a particular wavelength. This proposal is also a key idea of this thesis. At λ = 193 nm, this method was used to propose a feasible design to image high resolution structures, NA = 1.85 at an aspect ratio of ~3.2. To experimentally demonstrate the enhancements, a new type of solid immersion test bed, the solid immersion Lloyd's mirror interference lithography test-bed was constructed. High quality line and space patterns with a half-pitch of 55.5 nm were created using λ = 405 nm, corresponding to a NA of 1.824, that is well in the evanescent regime of light. Image depths of 33-40 nm were seen. Next, the evanescent image was coupled to an effective gain medium made up of a thin layer of hafnium oxide (HfO) upon silicon dioxide (SiO2). This resulted in a considerable depth enhancement, and 105 nm tall structures were imaged. The work in this thesis details the construction of the solid immersion lithography test-bed, describes the implementation of the modeling tools, details the theory and analysis required to achieve the relevant solutions and understanding of the physical mechanism and finally experimentally demonstrates an enhancement that allows evanescent interferometric lithography beyond conventional limits.