Accurate determination of the surface enhanced Raman scattering (SERS) enhancement factor (EF) is critically important for a fundamental understanding of the SERS phenomenon. Experimental quantification of SERS EFs is challenging. A series of instrument-, analyte-, and SERS-substrate related issues can affect the SERS intensity and thus compromise the reliability of the measured SERS EFs. This dissertation presents a series of computational and experimental studies that enhance the quantitative understanding of the SERS signal variation and identify ways to enhance the reliability of the SERS EF determination. Chapter I presents an overview of works described in this dissertation. The gold nanoparticle (AuNP) inner filter effect on SERS measurements is demonstrated in Chapter II. Using dithiopurine and ethanol as model analytes, we demonstrate that the nanoparticle will modify the analytes’ Raman signal through two competitive mechanisms: enhancing the Raman signal of the analyte on the nanoparticle surface through electromagnetic enhancement, and attenuating the analyte Raman signal through photon extinction. The significance of the AuNP inner filter effect is quantitatively evaluated using ethanol as the internal reference. A solvent internal reference method is presented in Chapter III for quantifying the SERS EFs of analytes adsorbed onto AuNPs and AgNPs. One of the key findings is that while an analyte’s SERS EF varies significantly as a function of nanoparticle aggregation, its peak SERS EF depends only on the types and sizes of nanoparticles, but not on experimental conditions including concentrations of analyte, nanoparticle, and aggregation reagent. Chapter IV presents a SERS internal reference method for the determination of the resonance Raman EFs in the SERS study of rhodamine 6G (R6G) adsorbed onto AuNPs and AgNPs. The most striking finding is that the AgNP binding reduces, instead of enhancing, the R6G resonance enhancement. Finally, the wavelength-dependent correlation between UV-vis intensities and SERS EFs of aggregated AuNPs and AgNPs were investigated under three fixed excitation wavelengths (532, 632, and 785 nm). The nanoparticle UV-vis intensity is an excellent indicator for identifying the optimal aggregation state for AgNP-based SERS acquisitions under each of the three excitation wavelengths and for the AuNP-based SERS under a 632 nm excitation.

Compared to single-mode VCSELs, multimode VCSELs have not received much attention in models and characterizations for functional parameters, despite making up the majority of commercially available VCSELs [1]. In particular, the extraction of the linewidth enhancement factor for multimode VCSELs has been overlooked, likely due to difficulties in measurement. Additionally, multimode models for VCSELs have, until recently, omitted spectral characteristics such as linewidth [2]. This is the first work to report a measured linewidth enhancement factor value (lower bound) for a multimode VCSEL. A characterization for the functional parameters of a red multimode vertical-cavity surface-emitting laser (VCSEL) is shown herein. The extracted values form a complete working set of parameters for the laser rate equations. The techniques employed for extracting values include frequency responses, power versus current fittings, and optical spectral measurements. From the frequency responses at various bias currents, the relaxation oscillation frequency and damping factor are found. The power versus current curve is fitted to find parameters including the modal spontaneous emission rate and carrier density at threshold. The spectral measurements are used for evaluating the linewidth enhancement factor (LEF) also known as the alpha factor or Henry factor. These 5 methods have been applied previously to characterizing single-mode VCSELs [3]–[5]. The experimentally extracted parameters herein are important for creating accurate models and simulations for multimode VCSELs. Improved multimode VCSEL models are necessary for improving optical communication, especially for short-range optical interconnects [2]. The measured parameters for the characterized VCSEL are comparable to similar single-mode VCSELs characterized in other works. This is promising because multi-mode VCSELs have higher output power than their single-mode counterparts, thus these results may aid in improving short-range optical interconnects.

A incorporação de nanopartículas metálicas em tecidos tumorais tem sido estudada em Radioterapia devido ao aumento de dose que pode ser obtido no volume alvo do tratamento. Estudos indicam que nanopartículas de ouro (AuNP) estão entre as de maior viabilidade biológica para essas aplicações, devido ao baixo potencial tóxico. Além disso, estudos mostram que AuNP de alguns nanômetros até alguns micrômetros podem permear vasos sanguíneos que alimentam tumores, permitindo sua incorporação nas células tumorais. Desta forma, este trabalho visou estudar os fatores de aumento de dose obtidos em Radioterapia com AuNP incorporadas ao tecido tumoral utilizando feixes de ortovoltagem, de braquiterapia e de teleterapia. Este trabalho utilizou de uma metodologia computacional, através de simulação Monte Carlo com o código PENELOPE. Foram simulados feixes clínicos de 50, 80, 150 e 250 kVp, Ir-192 e 6 MV, e um modelo de célula tumoral com AuNPs incorporadas com diferentes concentrações de ouro. O modelo de células utilizado possui 13 µm de diâmetro externo máximo e 2 µm de diâmetro no núcleo. Dois modelos de incorporação de AuNPs foram implementados: modelo homogêneo e modelo heterogêneo. No modelo homogêneo, as AuNP foram distribuídas homogeneamente no núcleo e as células foram irradiadas nas diferentes energias estudadas para avaliar o fator de aumento de dose (DEF) em função da concentração de ouro na célula e da energia do feixe. No modelo heterogêneo, aglomerados de AuNPs foram simulados individualmente dentro da célula. Neste modelo foram utilizados somente os espetros de radiação que apresentaram os melhores desempenhos no modelo homogêneo. Foram avaliadas a fluência de partículas ejetadas nas AuNPs, o DEF, as distribuições de doses e os perfis de dose com aglomerados de 50 a 220 nm na célula. Os resultados obtidos para o modelo homogêneo mostram que os feixes de baixa energia são os que proporcionam maior DEF para uma mesma concentração de AuNP. Os maiores DEFs obtidos foram de 2,80; 2,99; 1,62 e 1,61, para os feixes de 50 kVp, 80 kVp, 150 kVp, 250 kVp, respectivamente, sendo a maior incerteza de 1,9% para o feixe de 250 kVp. Através dos resultados obtidos com o modelo heterogêneo foi possível concluir que os elétrons ejetados possuem maior influência no aumento local da dose. Os perfis de dose, extraídos das distribuições de doses, para os aglomerados simulados permitiram obter os alcances das isodoses de 50, 20 e 10% da dose no entorno das AuNPs. Através desses perfis de dose pode-se concluir que o aumento de dose é local, da ordem de alguns micrômetros, dependendo do tamanho das nanopartículas e da energia do feixe primário. Para o feixe de 50 kVp, o DEF encontrado para uma incorporação heterogênea de seis aglomerados de AuNPs, correspondendo a um modelo clínico real, foi de 1,79, com incerteza de 0,4%. Com base nos resultados obtidos pode-se concluir que as energias de ortovoltagem proporcionam maior fator de aumento de dose que feixes de megavoltagem utilizados em teleterapia convencional. Além disso, o reforço local de dose pode proporcionar um fator de radiossensibilização celular se as AuNPs forem incorporadas no núcleo das células, nas redondezas do DNA, proporcionando um maior potencial de controle tumoral. / The incorporation of metal nanoparticles into tumor tissues has been studied in radiation therapy given of the dose enhancement that can be obtained in the target volume of the treatment. Studies indicate that gold nanoparticles (AuNP) are among the highest biologically viable for such applications, due to their low toxic potential. In addition, studies show that AuNP from a few nanometers to a few micrometers can permeate blood vessels that feed tumors, allowing their incorporation into tumor cells. Hence, this study´s goal was to study the dose enhancement factors obtained in radiation therapy with AuNP incorporated in the tumor using orthovoltage, brachytherapy and teletherapy beams. This work used a computational methodology, through Monte Carlo simulation with the PENELOPE package. Clinical beams of 50, 80, 150 and 250 kVp, Ir-192 and 6 MV were simulated with a tumor cell model with incorporated AuNPs. The cell model has maximum outer diameter of 13 m and 2 m of nucleus diameter. Two models of AuNP incorporation were implemented: homogeneous model and heterogeneous model. In the homogeneous model the AuNP were distributed homogeneously in the nucleus and the cells were irradiated in the different beams studied to evaluate the dose enhancement factors (DEF) as a function of concentration of gold in the cell and radiation beam. In the heterogeneous model, clusters of AuNPs were simulated individually within the cell. In this model, the radiation spectra used was selected among those that presented the best performances in the homogeneous model. The fluence of particles ejected from the AuNPs, the DEFs, the dose distributions and dose profiles for clusters of 50 to 220 nm in the cell were evaluated. The results obtained for the homogeneous model show that lower energy beams provide the highest DEFs for the same concentration of AuNP. The highest DEFs obtained were 2.80; 2.99; 1.62 and 1.61, for the beams of 50 kVp, 80 kVp, 150 kVp, 250 kVp, respectively, with a maximun uncertainty of 1.9% for the 250 kVp beam. Through the results obtained with the heterogeneous model it was possible to conclude that the electrons ejected from he AuNPs have the major influence on the local dose enhancement. The dose profiles extracted from the dose distributions for the simulated clusters allowed the evaluation of the ranges for the 50, 20 and 10% isodoses in the surroundings of the AuNPs. Through these dose profiles, it can be concluded that the dose increase is local, in the order of a few micrometers, depending on the size of the nanoparticles and the energy of the primary beam. For the 50 kVp beam, the DEF found for a heterogeneous incorporation of six clusters of AuNPs, corresponding to an actual clinical model, was 1.79, with uncertainty of 0.4%. Based on the results obtained it can be concluded that kilovoltage energies provide a higher dose enhancement factor than megavoltage beams used in teletherapy. In addition, local dose enhancement may provide a cellular radiosensitization factor if the nanoparticles are incorporated in the nucleus of the cells, in the vicinity of the DNA, providing an enhanced potential for tumor control.

ABSTRACT DETERMINATION OF CADMIUM USING SLOTTED QUARTZ TUBE ATOM TRAP ATOMIC ABSORPTION SPECTROMETRY AND METAL COATINGS &Ouml / zcan Gurbetoglu, G. Pelin M.S., Department of Chemistry Supervisor: Prof. Dr. O. Yavuz Ataman July 2010, 76 pages Flame atomic absorption spectroscopy (FAAS) is a common technique for detecting metals and metalloids in environmental, biological and metallurgical samples. Although it is a rather old technique, it is still very reliable, simple to use and inexpensive. The technique can be used to determine the concentration of over 70 different metals in a solution. However, it has detection limits at mg/L levels. Some atom trapping methods have been developed to reach the detection limits of ng/mL levels. Slotted quartz tube (SQT) is one of these atom trapping methods. It is an important technique, since it is easy to use, applicable in all laboratories, commercially available and economical. This thesis consists of development of a sensitive method for cadmium with the help of SQT atom trap. In this study, it was used for two different purposes. One was for keeping the analyte atoms more in the light path / in other words, for increasing the residence times of analyte atoms in the measurement zone. This first application was provided a 2.9 times enhancement with respect to conventional FAAS. Second application was for trapping the analyte on the surface of the SQT, in other words, for performing on-line preconcentration of cadmium in SQT. In the presence of a lean flame, analyte samples were trapped and collected for a few minutes at a low suction rate. After finishing the collection period, analyte atoms were revolatilized with the help of a small volume of (10-50 &micro / L) methyl isobutyl ketone (MIBK) and a rapid atomization occurred. This introduction also altered the flame composition momentarily and analyte atoms were released from the surface of the SQT. Application of this method enhanced the sensitivity 2065 times with respect to conventional FAAS. Another approach to this type of atom trapping has been investigated also in this study, which was coating of SQT with some metals having low volatility. Therefore, some transition metals were coated to the surface of SQT and among them zirconium was selected as the best coating material as having the most sensitivity enhancement factor. That is why, rest of the study was performed with the Zr coated SQT. The enhancement was 3368 as compared with FAAS. Cd determination with this method provides LOD value of 8 pg/mL and Co value of 19 pg/mL. In order to see the effect of some other type of elements or ions on determination of cadmium, interference study was done.

A incorporação de nanopartículas metálicas em tecidos tumorais tem sido estudada em Radioterapia devido ao aumento de dose que pode ser obtido no volume alvo do tratamento. Estudos indicam que nanopartículas de ouro (AuNP) estão entre as de maior viabilidade biológica para essas aplicações, devido ao baixo potencial tóxico. Além disso, estudos mostram que AuNP de alguns nanômetros até alguns micrômetros podem permear vasos sanguíneos que alimentam tumores, permitindo sua incorporação nas células tumorais. Desta forma, este trabalho visou estudar os fatores de aumento de dose obtidos em Radioterapia com AuNP incorporadas ao tecido tumoral utilizando feixes de ortovoltagem, de braquiterapia e de teleterapia. Este trabalho utilizou de uma metodologia computacional, através de simulação Monte Carlo com o código PENELOPE. Foram simulados feixes clínicos de 50, 80, 150 e 250 kVp, Ir-192 e 6 MV, e um modelo de célula tumoral com AuNPs incorporadas com diferentes concentrações de ouro. O modelo de células utilizado possui 13 µm de diâmetro externo máximo e 2 µm de diâmetro no núcleo. Dois modelos de incorporação de AuNPs foram implementados: modelo homogêneo e modelo heterogêneo. No modelo homogêneo, as AuNP foram distribuídas homogeneamente no núcleo e as células foram irradiadas nas diferentes energias estudadas para avaliar o fator de aumento de dose (DEF) em função da concentração de ouro na célula e da energia do feixe. No modelo heterogêneo, aglomerados de AuNPs foram simulados individualmente dentro da célula. Neste modelo foram utilizados somente os espetros de radiação que apresentaram os melhores desempenhos no modelo homogêneo. Foram avaliadas a fluência de partículas ejetadas nas AuNPs, o DEF, as distribuições de doses e os perfis de dose com aglomerados de 50 a 220 nm na célula. Os resultados obtidos para o modelo homogêneo mostram que os feixes de baixa energia são os que proporcionam maior DEF para uma mesma concentração de AuNP. Os maiores DEFs obtidos foram de 2,80; 2,99; 1,62 e 1,61, para os feixes de 50 kVp, 80 kVp, 150 kVp, 250 kVp, respectivamente, sendo a maior incerteza de 1,9% para o feixe de 250 kVp. Através dos resultados obtidos com o modelo heterogêneo foi possível concluir que os elétrons ejetados possuem maior influência no aumento local da dose. Os perfis de dose, extraídos das distribuições de doses, para os aglomerados simulados permitiram obter os alcances das isodoses de 50, 20 e 10% da dose no entorno das AuNPs. Através desses perfis de dose pode-se concluir que o aumento de dose é local, da ordem de alguns micrômetros, dependendo do tamanho das nanopartículas e da energia do feixe primário. Para o feixe de 50 kVp, o DEF encontrado para uma incorporação heterogênea de seis aglomerados de AuNPs, correspondendo a um modelo clínico real, foi de 1,79, com incerteza de 0,4%. Com base nos resultados obtidos pode-se concluir que as energias de ortovoltagem proporcionam maior fator de aumento de dose que feixes de megavoltagem utilizados em teleterapia convencional. Além disso, o reforço local de dose pode proporcionar um fator de radiossensibilização celular se as AuNPs forem incorporadas no núcleo das células, nas redondezas do DNA, proporcionando um maior potencial de controle tumoral. / The incorporation of metal nanoparticles into tumor tissues has been studied in radiation therapy given of the dose enhancement that can be obtained in the target volume of the treatment. Studies indicate that gold nanoparticles (AuNP) are among the highest biologically viable for such applications, due to their low toxic potential. In addition, studies show that AuNP from a few nanometers to a few micrometers can permeate blood vessels that feed tumors, allowing their incorporation into tumor cells. Hence, this study´s goal was to study the dose enhancement factors obtained in radiation therapy with AuNP incorporated in the tumor using orthovoltage, brachytherapy and teletherapy beams. This work used a computational methodology, through Monte Carlo simulation with the PENELOPE package. Clinical beams of 50, 80, 150 and 250 kVp, Ir-192 and 6 MV were simulated with a tumor cell model with incorporated AuNPs. The cell model has maximum outer diameter of 13 m and 2 m of nucleus diameter. Two models of AuNP incorporation were implemented: homogeneous model and heterogeneous model. In the homogeneous model the AuNP were distributed homogeneously in the nucleus and the cells were irradiated in the different beams studied to evaluate the dose enhancement factors (DEF) as a function of concentration of gold in the cell and radiation beam. In the heterogeneous model, clusters of AuNPs were simulated individually within the cell. In this model, the radiation spectra used was selected among those that presented the best performances in the homogeneous model. The fluence of particles ejected from the AuNPs, the DEFs, the dose distributions and dose profiles for clusters of 50 to 220 nm in the cell were evaluated. The results obtained for the homogeneous model show that lower energy beams provide the highest DEFs for the same concentration of AuNP. The highest DEFs obtained were 2.80; 2.99; 1.62 and 1.61, for the beams of 50 kVp, 80 kVp, 150 kVp, 250 kVp, respectively, with a maximun uncertainty of 1.9% for the 250 kVp beam. Through the results obtained with the heterogeneous model it was possible to conclude that the electrons ejected from he AuNPs have the major influence on the local dose enhancement. The dose profiles extracted from the dose distributions for the simulated clusters allowed the evaluation of the ranges for the 50, 20 and 10% isodoses in the surroundings of the AuNPs. Through these dose profiles, it can be concluded that the dose increase is local, in the order of a few micrometers, depending on the size of the nanoparticles and the energy of the primary beam. For the 50 kVp beam, the DEF found for a heterogeneous incorporation of six clusters of AuNPs, corresponding to an actual clinical model, was 1.79, with uncertainty of 0.4%. Based on the results obtained it can be concluded that kilovoltage energies provide a higher dose enhancement factor than megavoltage beams used in teletherapy. In addition, local dose enhancement may provide a cellular radiosensitization factor if the nanoparticles are incorporated in the nucleus of the cells, in the vicinity of the DNA, providing an enhanced potential for tumor control.

Due to the ever increasing concerns about pollutants and contaminants found in water, new treatment technologies have been developed. Ozonation is one of such technologies. It has been widely applied in the treatment of pollutants in water and wastewater treatment processes. Ozone has many applications such as oxidation of organic components, mineral matter, inactivation of viruses, cysts, bacteria, removal of trace pollutants like pesticides and solvents, and removal of tastes and odours. Ozone is the strongest conventional oxidant that can result in complete mineralisation of the organic pollutants to carbon dioxide and water. Because ozone is unstable, it is generally produced onsite in gas mixtures and is immediately introduced to water using gas/liquid type reactors (e.g. bubble columns). The ozone reactions are hence of the type gas liquid reactions, which are complex to model since they involve both chemical reactions, which occur in the liquid phase, and mass transfer from the gas to the liquid phase. This study focuses on two aspects: mass transfer and chemical reactions in multicomponent systems. The mass transfer parameters were determined by experiments under different conditions and the chemical reactions were studied using single component and multicomponent systems. Two models obtained from the literature were adapted to the systems used in this study. Mass transfer parameters in the semi-batch reactor were determined using oxygen and ozone at different flow rates in the presence and absence of t-butanol. t-Butanol is used as a radical scavenger in ozonation studies and it has been found to affect the gas-liquid mass transfer rates. An experimental study was carried out to investigate the effects of t-butanol concentrations on the physical properties of aqueous solutions, including surface tension and viscosity. It was found that t-butanol reduced both properties by 4% for surface tension and by a surprising 30% for viscosity. These reductions in the solution physical properties were correlated to enhancement in the mass transfer coefficient, kL. The mass transfer coefficient increased by about 60% for oxygen and by almost 50% for ozone. The hydrodynamic behaviour of the system used in this work was characterised by a homogeneous bubbling regime. It was also found that the gas holdup was significantly enhanced by the addition of t-butanol. Moreover, the addition of t-butanol was found to significantly reduce the size of gas bubbles, leading to enhancement in the volumetric mass transfer coefficient, kLa. The multicomponent ozonation was studied with two systems, slow reactions when alcohols were used and fast reactions when endocrine disrupting compounds were used. ii These experiments were simulated by mathematical models. The alcohols were selected depending on their volatilization at different initial concentrations and different gas flow rates. The degradation of n-propanol as a single compound was studied at the lowest flow rate of 200 mL/min. It was found that the degradation of n-propanol reached almost 60% within 4 hours. The degradation of the mixture was enhanced with an increase in the number of components in the mixture. It was found that the degradation of the mixture as three compounds reached almost 80% within four hours while the mixture as two compounds reached almost 70%. The effect of pH was studied and it was found that an increase in pH showed slight increase in the reaction. Fast reactions were also investigated by reacting endocrine disrupting chemicals with ozone. The ozone reactions with the endocrine disrupters were studied at different gas flow rates, initial concentrations, ozone concentrations and pH. The degradation of 17β-estradiol (E2) as a single compound was the fastest, reaching about 90% removal in almost 5 minutes. However estrone (E1) degradation was the lowest reaching about 70% removal at the same time. The degradation of mixtures of the endocrine disruptors was found to proceed to lower percentages than individual components under the same conditions. During the multicomponent ozonation of the endocrine disruptors, it was found that 17β-estradiol (E2) converted to estrone (E1) at the beginning of the reaction. A MATLAB code was developed to predict the ozone water reactions for single component and multicomponent systems. Two models were used to simulate the experimental results for single component and multicomponent systems. In the case of single component system, good simulation of both reactions (slow and fast) by model 1 was obtained. However, model 2 gave good agreement with experimental results only in the case of fast reactions. In addition, model 1 was applied for multicomponent reactions (both cases of slow and fast reaction). In the multicomponent reactions by model 1, good agreement with the experimental results was also obtained for both cases of slow and fast reactions.

In the quest for reliable, repeatable and stable field electron emission that has commercial potential, whilst many attempts have been made, none yet has been truly distinguishable as being successful. Whilst I do not claim within this thesis to have uncovered the secret to success, fundamental issues have been addressed that concern the future directions towards achieving its full potential. An exhaustive comparison is made across the diverse range of materials that have, over the past 40-50 years, been postulated and indeed tested as field emitters. This has not previously been attempted. The materials are assessed according to the important metrics of turn on voltage, Eon, and maximum current density, Jmax, where low Eon and high Jmax are seen as desirable. The nano-carbons, carbon nanotubes (CNTs), in particular, perform well in both these metrics. No dependency was seen between the material work function and its performance as an emitter, which might have been suggested by the Fowler Nordheim equations. To address the issues underlying the definition of the local enhancement factor, β, a number of variations of surface geometry using CNTs were fabricated. The field emission of these emitters was measured using two different approaches. The first is a Scanning Electrode Field Emission Microscope, SAFEM, which maps the emission at individual locations across the surface of the emitter, and the parallel plate that is more commonly encountered in field emission measurements. Finally, an observed hysteretic behaviour in CNT field emission was explored. The field emitters were subjected to a number of tests. These included; in-situ residual gas analysis of the gas species in the emitter environment, a stability study in which the emitters were exposed to a continuing voltage loop for 50 cycles, differing applied voltage times to analyse the effects on the emitted current, and varying maximums of applied field in a search for hysteresis onset information. These studies revealed the candidate in causing the hysteresis is likely to be water vapour that adsorbs on the CNT surface. A six step model if the emission process was made that details how and when the hysteresis is caused.

This diploma thesis deals with the design and optimization of the device for measurement of field emission from gallium nitride (GaN) nanocrystals surface. The first part of the thesis is the topic review, which contains the introduction to the problematics of field emissio focused on GaN. Then there were designed, constructed and optimized two versions of the device for the measurement of field emission. Through the optimization phase, the first successful test has been performed with zinc oxide (ZnO) nanowires. Simultaneously GaN nanocrystals were fabricated on the silicon substrate Si(111) with 2 nm of silicon dioxide SiO2 and also on the copper foil covered by graphene by molecular beam epitaxy (MBE). In the last chapter, there are presented the results of the measurement for emission of GaN nanocrystals. Finally, this study is comparing results with the current research in the area of field emission, which displays the improved characteristics for field emission of GaN nanocrystals on the copper foil covered by graphene.

Due to the ever increasing concerns about pollutants and contaminants found in water, new treatment technologies have been developed. Ozonation is one of such technologies. It has been widely applied in the treatment of pollutants in water and wastewater treatment processes. Ozone has many applications such as oxidation of organic components, mineral matter, inactivation of viruses, cysts, bacteria, removal of trace pollutants like pesticides and solvents, and removal of tastes and odours. Ozone is the strongest conventional oxidant that can result in complete mineralisation of the organic pollutants to carbon dioxide and water. Because ozone is unstable, it is generally produced onsite in gas mixtures and is immediately introduced to water using gas/liquid type reactors (e.g. bubble columns). The ozone reactions are hence of the type gas liquid reactions, which are complex to model since they involve both chemical reactions, which occur in the liquid phase, and mass transfer from the gas to the liquid phase. This study focuses on two aspects: mass transfer and chemical reactions in multicomponent systems. The mass transfer parameters were determined by experiments under different conditions and the chemical reactions were studied using single component and multicomponent systems. Two models obtained from the literature were adapted to the systems used in this study. Mass transfer parameters in the semi-batch reactor were determined using oxygen and ozone at different flow rates in the presence and absence of t-butanol. t-Butanol is used as a radical scavenger in ozonation studies and it has been found to affect the gas¿liquid mass transfer rates. An experimental study was carried out to investigate the effects of t-butanol concentrations on the physical properties of aqueous solutions, including surface tension and viscosity. It was found that t-butanol reduced both properties by 4% for surface tension and by a surprising 30% for viscosity. These reductions in the solution physical properties were correlated to enhancement in the mass transfer coefficient, kL. The mass transfer coefficient increased by about 60% for oxygen and by almost 50% for ozone. The hydrodynamic behaviour of the system used in this work was characterised by a homogeneous bubbling regime. It was also found that the gas holdup was significantly enhanced by the addition of t-butanol. Moreover, the addition of t-butanol was found to significantly reduce the size of gas bubbles, leading to enhancement in the volumetric mass transfer coefficient, kLa. The multicomponent ozonation was studied with two systems, slow reactions when alcohols were used and fast reactions when endocrine disrupting compounds were used. ii These experiments were simulated by mathematical models. The alcohols were selected depending on their volatilization at different initial concentrations and different gas flow rates. The degradation of n-propanol as a single compound was studied at the lowest flow rate of 200 mL/min. It was found that the degradation of n-propanol reached almost 60% within 4 hours. The degradation of the mixture was enhanced with an increase in the number of components in the mixture. It was found that the degradation of the mixture as three compounds reached almost 80% within four hours while the mixture as two compounds reached almost 70%. The effect of pH was studied and it was found that an increase in pH showed slight increase in the reaction. Fast reactions were also investigated by reacting endocrine disrupting chemicals with ozone. The ozone reactions with the endocrine disrupters were studied at different gas flow rates, initial concentrations, ozone concentrations and pH. The degradation of 17¿-estradiol (E2) as a single compound was the fastest, reaching about 90% removal in almost 5 minutes. However estrone (E1) degradation was the lowest reaching about 70% removal at the same time. The degradation of mixtures of the endocrine disruptors was found to proceed to lower percentages than individual components under the same conditions. During the multicomponent ozonation of the endocrine disruptors, it was found that 17¿-estradiol (E2) converted to estrone (E1) at the beginning of the reaction. A MATLAB code was developed to predict the ozone water reactions for single component and multicomponent systems. Two models were used to simulate the experimental results for single component and multicomponent systems. In the case of single component system, good simulation of both reactions (slow and fast) by model 1 was obtained. However, model 2 gave good agreement with experimental results only in the case of fast reactions. In addition, model 1 was applied for multicomponent reactions (both cases of slow and fast reaction). In the multicomponent reactions by model 1, good agreement with the experimental results was also obtained for both cases of slow and fast reactions. / Ministry of Higher Education in Libya and the Libyan Cultural Centre and Educational Bureau in London.

This thesis reports an experimental characterization of the ultrafast gain and refractive index dynamics of a novel InAs/InGaAsP/InP quantum-dot (QD) semiconductor optical amplifier (SOA) operating near 1.55-µm wavelengths, assessing its high-speed performance characteristics for the first time. The thesis also studies the influence of the degree of quantum confinement on the dynamics of SOAs by comparing the zero-dimensional (0-D) QD's dynamics to those in 1-D InAs/InAlGaAs/InP quantum-dash (QDash), and 2-D InGaAsP/InGaAsP/InP quantum-well (QW) SOAs, both of which also operate near 1.55-µm wavelengths, and are made with matching or similar materials and structures. The ultrafast (around 1 ps) and long-lived (up to 2 ns) amplitude and phase dynamics of the SOAs are characterized via advanced heterodyne pump-probe measurements with 150-femtosecond resolution. It is found that the QD SOA has an 80-picosecond amplitude, and 110-picosecond phase recovery lifetime in the gain regime, 4-6 times faster than the QDash and QW recovery lifetimes, as well as reduced ultrafast transients, giving it the best properties for high-speed (> 100 Gb/s) all-optical signal processing in the important telecommunications wavelength bands. An impulse response model is developed and used to analyze the dynamics, facilitating a comparison of the gain compression factors, time-resolved linewidth enhancement factors (alpha-factors), and instantaneous dynamic coefficients (two-photon absorption and nonlinear refractive-index coefficients) amongst the three structures. The quantum-dot device is found to have the lowest effective alpha-factor, 2-10, compared to 8-16 in the QW, as well as time-resolved alpha-factors lower than in the QW—promising for reduced-phase-transient operation at high bitrates. Significant differences in the alpha-factors of lasers with the same structure are found, due to the differences between gain changes that are induced optically or through the electrical bias. The relative contributions of stimulated transitions and free-carrier absorption to the total carrier heating dynamics in SOAs of varying dimensionality are also reported for the first time. Examining the QD electroluminescence and linear gain spectra in combination with the carrier dynamics also brings about conclusions on the nature of the quantum confinement, dot energy-level structure, and density of states—aspects of the material that have not been previously well understood.