Designs for deep ultraviolet (DUV) edge emitting laser diodes (LDs) based on the wurtzite III-nitride (III-N) material system are presented. A combination of proprietary and commercial advanced semiconductor LD simulation software is used to study the operation of III-N based DUV LDs theoretically. Critical factors limiting device performance are identified based on an extensive literature survey. A comprehensive design parameter space is investigated thoroughly with the help of advanced scripting capabilities. Several design strategies are proposed to eliminate the critical problems completely or partially. A DUV LD design is proposed based exclusively on AlInN active layers grown epitaxially on bulk AlN substrates because AlInN offers a promising alternative to AlGaN for the realization of LDs and LEDs operating in the DUV regime. The proposed AlInN-based design also features a tapered electron blocking layer (EBL) instead of a homogeneous one. Tapered EBLs redistribute the interfacial polarization charge volumetrically throughout the entire EBL thickness via compositional grading, and eliminate the parasitic inversion layer charge. AlGaN based DUV LD designs are explored also because at present, it may be difficult to grow AlInN epitaxially with superior crystalline quality. Polarization charge matching is proposed to improve electron and hole wavefunction overlap within the active region. Although the strategy of polarization charge matching has already been proposed in the literature to enhance performance of visible wavelength LEDs and LDs, the proposed design presents the first demonstration that polarization charge matching is also feasible for DUV LDs operating at sub-300 nm wavelengths. A lateral current injection (LCI) LD design is proposed featuring polarization-charge-matched barriers and regrown Ohmic contacts to avoid a group of issues related to the highly inefficient p-type doping of wide bandgap III-N materials in vertical injection designs. The proposed design partially decouples the problem of electrical injection from that of optical confinement. Although the idea of an LCI LD design has been proposed in the literature in the 90s to be used as longer wavelength active sources in optoelectronic integrated circuits using GaInAsP/InP and related material systems, the proposed design is the first theoretical demonstration that this concept can be applied to DUV LDs based on III-N material system. To solve the problem of hole transport in vertical injection designs, a DUV LD design based exclusively on AlGaN material system is presented, featuring an inverse-tapered p-waveguide layer instead of an EBL. Several EBL designs are investigated, and compared with conventionally-tapered EBL design. Through judicious volumetric redistribution of fixed negative polarization charge, inverse tapering may be exploited to achieve nearly flat valence band profiles free from barriers to hole injection into the active region, in contrast to conventional designs. Numerical simulations demonstrate that the inverse tapered strategy is a viable solution for efficient hole injection in vertical injection DUV LDs operating at shorter wavelengths (< 290 nm).

Fundação de Amparo a Pesquisa do Estado de Minas Gerais / The SNABP [40SiO2.30Na2CO3.1Al2O3.25B2O3.PbO2 (mol%)] glass system, nanostructured with PbS Quantum Dots (QDs) and/or doped with Er3+ ions, was successfully synthesized by the Fusion Method, when it was subjected to appropriate thermal annealing. The glass transition temperatures (Tg) were obtained by Differential Thermal Analyze (DTA), in which it was possible to define a suitable temperature to be used in the thermal annealing of the synthesized samples. As results of these thermal annealing, the formation and growth of PbS QDs have occurred in the glass environment. The optical properties of samples were investigated by Optical Absorption (OA), Photoluminescence (PL), and Photoluminescence with Temporal Resolution (PLTR). Moreover, the Atomic Force Microscopy (AFM) and X-Ray Diffractometry were employed in study of morphological and structural properties of samples, respectively. The size dispersions of PbS QDs were determined from OA spectra. Once using both the Method and OA data, it was also possible to estimate the average diameters of these nanoparticles, which grow with the increase in annealing time. The characteristic transitions of Er3+ ions were clearly identified in OA spectra. In addition, it was observed that the increase in annealing time of samples had provoked amplification in the overlapping between PL bands of both the PbS QDs and Er3+ ions, as well as with the absorption 4I15/2 -> 4I13/2 of these ions. Thus, the PLTR measurements have confirmed the decrease in lifetime of the 4I13/2 level (of Er3+ ions), with the amplification in the overlapping of PL emissions. Finally, as a main result of this work, it was proved that the SNABP glass system, nanostructured with PbS QDs and doped with Er3+ ions, displays to be quite favorable to the radiative energy transfer process (from PbS QDs to Er3+ ions), as well as the occurrence of stimulated emission of 4I13/2 level. / O sistema vítreo SNABP [40SiO2.30Na2CO3.1Al2O3.25B2O3.PbO2 (mol%)] nanoestruturado com pontos quânticos (PQs) de PbS e/ou dopados com íons Er3+ foi sintetizado com sucesso pelo Método de Fusão, quando submetido a tratamentos térmicos apropriados. As temperaturas de transição vítrea (Tg) foram obtidas por Análise Térmica Diferencial (DTA), em que foi possível definir uma temperatura adequada para ser utilizada nos tratamentos térmicos das amostras sintetizadas. Como resultados desses tratamentos térmicos, a formação e crescimento dos PQs de PbS ocorreram no ambiente vítreo. As propriedades ópticas das amostras foram investigadas por Absorção Óptica (AO), Fotoluminescência (PL) e Fotoluminescência com Resolução Temporal (PLRT). Além disso, a Microscopia de Força Atômica (AFM) e Difratometria de Raios-X (DRX) foram empregadas no estudo das propriedades morfológicas e estruturais das amostras, respectivamente. As dispersões de tamanho dos PQs de PbS foram determinadas a partir dos espectros de AO. Com a utilização do Método e os dados de AO, foi também possível estimar os diâmetros médios dessas nanopartículas, que aumentaram com o aumento no tempo de tratamento térmico. As transições características dos íons Er3+ foram claramente identificadas nos espectros de AO. Em adição, foi observado que o aumento no tempo de tratamento das amostras provocou um aumento na sobreposição entre as bandas de PL dos PQs de PbS e dos íons Er3+, bem como com a absorção 4I15/2 -> 4I13/2 desses íons. Assim, as medidas de PLRT confirmaram o decréscimo no tempo de vida do nível 4I13/2 (dos íons Er3+) com o aumento dessa sobreposição das emissões de PL. Finalmente, como principal resultado deste trabalho, foi comprovado que o sistema vítreo SNABP nanoestruturado com PQs de PbS dopados com íons Er3+ mostrou-se bastante favorável ao processo de transferência de energia radiativa (dos PQs de PbS para os íons Er3+), bem como a ocorrência da emissão estimulada do nível 4I13/2. / Mestre em Física

Fundação de Amparo a Pesquisa do Estado de Minas Gerais / In this work, Zn1-xAxTe (A = Mn, Co) diluted magnetic semiconductors (DMS) nanocrystal (NCs) were successfully grown in the P2O5 ZnO Al2O3 BaO PbO glass system synthesized by the method of Fusion-Nucleation, after subjecting to appropriate thermal annealing. Various experimental techniques were used in this study in order to get a comprehensive understanding of the optical, morphological, structural and magnetic properties these NCs. Transmission electron microscopy (TEM) and atomic force microscopy (AFM) images revealed the size of both of Zn1-xMnxTe and Zn1-xCoxTe NCs. From the vibrating sample magnetometer (VSM) technique, there was growth behavior of magnetization and magnetic susceptibility as a function of the Mn concentration in the samples containing Zn1-xMnxTe NCs. At lower Mn concentrations, the sp electrons of ZnTe host semiconductor interact with the d electrons of Mn2+ ions, resulting in the sp-d exchange interaction, which causes a small increase in susceptibility. At higher Mn concentrations, the d-d exchange interaction between Mn atoms dominates over the sp-d exchange interaction, resulting in an abrupt increase in susceptibility. The EPR spectra, in addition to prove the results exhibited the well-known sextet hyperfine lines of Mn2+ ions, since samples with low Mn concentrations revealed the presence of Mn2+ ions within and near the surface of the ZnTe NCs. From the optical absorption spectra (OA) and photoluminescence (PL), analyzed on the basis of crystal field theory (CFT) as well as of the diffraction X-ray (XRD), Raman scattering (RS) and electron microscopy transmission (TEM) techniques, the substitutional incorporation of Mn2+ ions was confirmed up to its solubility limit (x = 0.100) ZnTe NCs. Above this concentration, can observe the formation of manganese oxide NCs such as MnO and MnO2, since the nucleation rate for the formation of these NCs is greater than that of Zn1-xMnxTe NCs, at high concentrations. Furthermore, from the PL spectra, it was found that it is possible to tune the emission of energy related to transition 4T1(4G) &#8594; 6A1(6S) of Mn2+ ions, of the spectral orange region to the near infrared, depending on Mn concentration. This is possible due to the variation of the local crystal field, where these ions are inserted. From the OA spectra, analyzed on the basis of CFT, it showed that Co2+ ions are substitutionally incorporated in tetrahedral sites of ZnTe NCs, due to its characteristics transitions in visible and near infrared spectral region. This evidence has been enhanced from MFM images, since NCs doped with magnetic ions, magnetically respond when induced by the magnetization of the probe. / Neste trabalho, nanocristais semicondutores magnéticos diluídos (SMD) de Zn1-xAxTe (A = Mn; Co) foram crescidos com sucesso no sistema vítreo P2O5 ZnO Al2O3 BaO PbO, sintetizado pelo método de Fusão-Nucleação, após submetê-lo a tratamento térmico apropriado. Várias técnicas experimentais foram utilizadas neste estudo a fim de obter um entendimento compreensivo das propriedades ópticas, morfológicas, estruturais e magnéticas desses NCs. Imagens de microscopia eletrônica de transmissão (MET) e microscopia de força atômica (MFA) revelaram o tamanho tanto de NCs de Zn1-xMnxTe quanto de Zn1-xCoxTe. A partir da técnica de magnetometria de amostra vibrante (MAV), verificou-se o crescimento da magnetização e o comportamento da susceptibilidade magnética, em função da concentração de Mn, em amostras contendo NCs de Zn1-xMnxTe. Em baixas concentrações de Mn, os elétrons sp do semicondutor hospedeiro ZnTe, interagem com os elétrons d dos íons Mn2+, resultando na interação de troca sp-d, que provoca um pequeno aumento na susceptibilidade magnética. Já, em concentrações mais elevadas de Mn, a interação de troca d-d entre átomos de Mn domina a interação de troca sp-d, o que resulta em um aumento abrupto da susceptibilidade. Os espectros RPE, além de comprovar esses resultados, exibiram o bem conhecido sexteto de linhas hiperfinas de íons Mn2+, uma vez que amostras com baixas concentrações de Mn revelaram a presença de íons Mn2+ no interior e próximos à superfície dos NCs de ZnTe. A partir dos espectros de absorção óptica (AO) e fotoluminescência (FL), analisados com base na teoria do campo cristalino (TCC), bem como das técnicas de difração de raios-X (DRX), espalhamento Raman (ER) e microscopia eletrônica de transmissão (MET), confirmou-se a incorporação substitucional de íons Mn2+ até seu limite de solubilidade nominal (x = 0,100) em NCs de ZnTe. Acima dessa concentração, observa-se a formação de NCs de óxido de manganês, tais como MnO e MnO2, uma vez que a taxa de nucleação para a formação desses NCs é maior que a de NCs de Zn1-xMnxTe, em altas concentrações. Além disso, a partir dos espectros FL, verificou-se que é possível sintonizar a energia de emissão relacionada à transição 4T1(4G) &#8594; 6A1(6S) de íons Mn2+, da região espectral laranja ao infravermelho próximo, em função da concentração de Mn. Isso é possível devido à variação do campo cristalino local, onde esses íons estão inseridos. A partir dos espectros AO, analisados com base na TCC, evidenciou-se que íons Co2+ são incorporados substitucionalmente em sítios tetraédricos de NCs de ZnTe, devido às suas transições características na região espectral do visível e infravermelho próximo. Essa evidência foi reforçada a partir de imagens de MFM, uma vez que os NCs, dopados com íons magnéticos, respondem magneticamente quando induzidos pela magnetização da sonda. / Doutor em Física

Vidros teluritos são considerados fortes candidatos para aplicações em lasers e óptica não linear devido a importantes características, como o elevado índice de refração, baixa energia de fônons, baixa temperatura de transição vítrea e sua fácil preparação. Neste trabalho foram produzidas amostras dos sistemas vítreos TeO2- ZnO-Na2O, TeO2-Nb2O5-Na2O e Te2O-Na2O incluindo ou não dopagens de AgNO3 para estudos estruturais e ópticos. As propriedades estruturais e os mecanismos de recombinação destes vidros foram estudados por meio das técnicas de ressonância paramagnética eletrônica, termoluminescência e correntes de despolarização termicamente estimuladas. Já as propriedades ópticas como o coeficiente de absorção linear, índice de refração linear e não linear foram estudadas por meio das técnicas de absorção óptica, acoplamento de prismas e varredura Z. Foram ainda desenvolvidos estudos da precipitação de nanopartículas de prata para o sistema TeO2-ZnO-Na2O com dopagens de AgNO3 com diferentes temperaturas de tratamento térmico. A caracterização das nanopartículas metálicas foi realizada por meio da técnica de absorção óptica auxiliada por microscopia eletrônica de transmissão e espectrometria de energia dispersiva. Foram observadas por ressonância paramagnética eletrônica quatro respostas paramagnéticas dos vidros irradiados com raio , sendo uma de natureza desconhecida e as outras três identificadas como g¹, g² e g³ atribuídas respectivamente ao centro de buraco do telúrio e do oxigênio, centro de buraco do oxigênio terminal e centro de elétron do telúrio. Foi proposto ainda um modelo para explicar os mecanismos de formação destes centros. A partir dos resultados de termoluminescência observou-se que os processos de recombinação destes centros de defeitos são não radioativos. Neste projeto foram estudados pela primeira vez na literatura os fenômenos de polarização e despolarização em vidros teluritos, com e sem irradiação gama, por meio da técnica de correntes de despolarização termicamente estimuladas. Quanto às propriedades ópticas, foi investigada a influência da adição de prata dos sistemas vítreos TeO2-ZnO-Na2O e TeO2-Nb2O5-Na2O em relação à energia do gap, a cauda de Urbach, índice de refração linear e não linear.Nos resultados de varredura Z do sistema vítreo TeO2-Nb2O5-Na2O foi observado o aumento da assimetria na curva com aumento da adição de AgNO3 Este fenômeno foi explicado por meio de uma adaptação do modelo de Sumi para processos não radiativos, responsáveis pelo aumento do caráter térmico do índice de refração não linear. Por fim um modelo foi criado para explicar a precipitação de nanopartículas de prata na matriz vítrea TeO2-ZnO-Na2O mediante tratamento térmico. / Tellurite glasses are considered powerful candidates for applications in lasers and nonlinear optics due to their important properties such as high refractive index, low phonon energy, relatively low glass transition temperature and easy glass production at room atmosphere. In this work glass samples of the systems ZnO-Na2O, TeO2-Nb2O5-Na2O and Te2O-Na2O were produced, including or not the AgNO3 doping for the structural and optical study purposes. The structural properties and the recombination mechanisms of these glasses were studied by means of the techniques of electron paramagnetic resonance, thermoluminescence and thermally stimulated depolarization currents. The optical properties such as the optical linear absorption coefficient, linear and nonlinear refractive index were studied by means of the optical absorption techniques, prism coupling and Z-scan. Further studies were developed on the precipitation of silver nanoparticles embedded in the glass system TeO2-ZnO-Na2O doped with AgNO3, by means of thermal treatments at different temperatures. The characterization of the metallic nanoparticles was carried out by optical absorption aided by transmission electron microscopy and dispersive energy spectroscopy. Four paramagnetic responses were observed by electron paramagnetic resonance of the -irradiated glasses, one not yet identified and the other three identified as g0, g1 and g3 attributed respectively to the tellurium-oxygen hole center, non-bridging oxygen hole center and tellurium electron center. A model to explain the formation mechanisms of these centers was proposed. The thermoluminescence results indicated that the recombination processes of these centers are non-radiative. This is the first study that deals with polarization and depolarization phenomena in tellurite glasses with and without gamma irradiation, by the technique of thermally stimulated depolarization currents. In what regards the optical properties of the glass systems TeO2-ZnONa2O and TeO2-Nb2O5-Na2O, the effect of the silver doping on the gap energy, Urbach tail, linear and nonlinear refractive indices were investigated. Through the Z-scan technique results of the glass system TeO2-Nb2O5-Na2O, an increasing asymmetry of the curve, with increasing AgNO3 content was observed. This phenomenon was explained through an adaptation of Sumi´s model for non-radiative processes, applied to a silver doped insulating glass, to explain the thermal character of the nonlinear refractive index. Finally, a model was developed to explain the silver nanoparticles precipitation in the TeO2-ZnO-Na2O glass matrix submitted to thermal treatment.

Quasi-particles formed in lithium niobate after pulse exposure were investigated by transient absorption and photoluminescence spectroscopy as well as numerical simulations. This includes the formation process, the transport through the crystal, interim pinning on defects during the relaxation process, and the final recombination with deep centers. It was shown that the charge-transport through the crystal can be described by a hopping transport including different types of hops between regular or defective lattice sites, i.e., the transport includes a mixture of free and bound small polarons. Furthermore, the different types of hops connected with varying activation energies and their distribution are responsible for an altered temporal decay curve when changing the crystal composition or temperature. Additionally, it was shown that the hitherto accepted recombination model is insufficient to describe all transient absorption and luminescence effects in lithium niobate under certain experimental conditions, i.e., long-living absorption dynamics in the blue/UV spectral range do not follow the typical polaron dynamics and cannot be described under the assumption of charge compensation. However, similar decay characteristics between self-trapped excitons known from photoluminescence spectroscopy and the unexpected behavior of the transient absorption were found leading to a revised model. This includes, besides the known polaron relaxation and recombination branch, a significant role of self-trapped excitons and their pinning on defects (pinned STEs). Since the consideration of further absorption centers in the relaxation path after pulse exposure might result in misinterpretations of previously determined polaron absorption cross-sections and shapes, the necessity to perform a review became apparent. Therefore, a supercontinuum pump-probe experiment was designed and all measurements applied under the same experimental conditions (temperature, polarization) so that one can extract the absorption amplitudes of the single quasi-particles in a spectral range of 0.7-3.0eV. The detailed knowledge might be used to deconvolve the absorption spectra and transform them to number densities of the involved centers which enables one to obtain an easier insight into recombination and decay dynamics of small polarons and self-trapped excitons. As the hopping transport of quasi-particles and the concept of pinned STEs might be fundamental processes, a thorough understanding opens up the possibility of their exploitation in various materials. In particular, results presented herein are not only limited to lithium niobate and its applications; an extension to a wide range of further strongly polar crystals in both their microscopic processes and their use in industry can be considered.

"Laser flash spectroscopy of photosystem II" Photosystem II (PS II) of plants and cyanobacteria oxidizes water in a light-powered reaction. Thereby, this protein is the ultimate source of the atmospheric oxygen. The capacity to oxidize water is owed to two properties of PS II: (i) The midpoint potential of the oxidizing chlorophyll moiety is increased by 0.6 V compared to photosystem I or photochemical reaction centers of anoxygenic bacteria, and (ii) the energy requirements of the four steps needed for the tetravalent oxidation of water are adapted to the energy of red light quanta. This thesis deals with two particular aspects, namely: 1. The coupling of the electron transfer from tyrosine Z (YZ) to the primary donor (P680+) to proton transfer, and an inquiry on the role of a positive charge on YZox (plus base cluster) in increasing the oxidizing potential at the catalytic site. 2. The localization of the electron hole, P680+, among the excitonically coupled four inner chlorophyll a molecules, and an estimation of the midpoint potential differences between them. Electron-proton-coupling by YZ This study was carried out with PS II core complexes from spinach or pea with a deactivated (removed) manganese cluster. The reduction of P680+ was investigated as a function of pH by detecting the laser flash induced absorption changes with nanosecond resolution. Two kinetic components were found with different pH-dependence and activation energies. The alteration of kinetic parameters by H/D isotope substitutions or by addition of divalent cations implied two different types of YZ-oxidation: At acidic pH the electron transfer was coupled with proton transfer, whereas in the alkaline region it was more rapid and no longer controlled by proton transfer. The conversion between both mechanisms occured at pH 7.4. This value corresponds either to the apparent pK of YZ itself (i.e. of the hydroxy group of the phenol ring) or to the pK of an acid-base-cluster, which includes YZ. Independent measurements of pH-transients by following the absorption changes of hydrophilic proton indicators corroborated this notion. The data were interpreted as indicating that the phenolic proton of YZ was released into the medium at acidic, but not at alkaline pH. The electron transfer and proton release characteristics of intact, oxygen-evolving PS II resembled those in deactivated samples kept at alkaline pH. We concluded that the electron transfer from YZ to P680+ in the native system was not coupled with proton transfer into the bulk. This has shed doubt on a popular hypothesis on the role of YZ as 'hydrogen abstractor' from bound water. On the other hand, the energetic constraints of water oxidation could be eased by the positive upcharging during oxidation of YZox plus its base cluster. On the localization of the electron hole of P680+ Photooxidation of PS II oxidizes the set of four innermost chlorophyll a molecules giving rise to the only spectroscopically defined species P680+. The deconvolution of difference spectra into bands of pigments is ambiguous. By using photoselective excitation of antennae, i.e. chl a molecules with site specific energies at the long wavelength border of the mean Qy-band, and by polarized detection, it was possible to tag P680+QA-/P680QA and 3P680/P680 difference spectra with a further parameter, the (wavelength-dependent) anisotropy r. Results obtained at liquid nitrogen temperature (77 K) can be clearly interpreted in terms of two chl a monomer bands. The two main components of the P680+QA-/P680QA difference spectrum were marked by two distinct values of the anisotropy and could be interpreted in a straightforward manner: the bleaching of a band at 675 nm belonging to the charged species (chl a+) and an electrochromic blue-shift of a nearby chl a from 684 to 682 nm. The main bleaching band of the 3P680/P680 spectrum (at 77 K) can be apparently attributed to a third (or several) chl a component(s). The analysis of the P680+QA-/P680QA spectrum at cryogenic temperature is compatible with monomeric chl a bands. On the other hand, one could assume a system of excitonically coupled core pigments, as it was recently introduced in the literature on the basis of energy transfer studies ('multimer model'). However, in view of the clear indications for an electrochromic band shift and the location of the bleaching band, which absorbs in a wavelength region of monomeric chl a, one assumption of the 'multimer model' should be questioned. Presumably, the excitonic couplings are rather weak, in particular between each of the two central chl a-molecules (PA/PB) and its respective accessory chl a (BA/BB), because of (i) the distances and (ii) different site energies of the monomeric chromophores. At room temperature, the absorption difference and anisotropy spectra of P680+QA-/P680QA were clearly altered. The anisotropy data indicated that the changes could no longer exclusively be ascribed to thermal broadening of individual bands. The localization of the positive charge on one pigment, analogous to the situation at 77 K, was now unlikely. Hence, the midpoint potential differences between the inner four chlorophyll a molecules were small and were estimated as approximately 15 meV.