No presente trabalho, realizado com hemoproteínas na forma de pó, o efeito da hidratação foi observado através de espectroscopia fotoacústica. Amostras de carboxi-hemoglobina e carboxi-mioglobina mantidas em diferentes ambientes de umidade relativa (UR), mostraram variações em seus espectros na região da banda de Soret. Para amostras mantidas em baixa hidratação característico do derivado carboxi, em alta hidratação (acima de aproximadamente 90% UR) o espectro era característico do derivado carboxi e na região intermediária o espectro era de uma mistura dos dois derivados. Essa mudança de ligante observada em alta hidratação pode ser explicada supondo que a proteína tem flexibilidade e atinge um estado conformacional que possibilita a entrada e saída do ligante. Em baixa hidratação a estrutura da proteína é rígida e tal que o acesso ao grupo heme está fechado, impossibilitando a troca do ligante. Essa explicação é coerente com vários resultados experimentais que indicam a existência de duas estruturas para essas hemoproteínas em solução / At the present work accomplished with powder of hemoproteins, the hydration effect was observed through photoacoustic spectroscopy. Samples of caroxyhemoglobin and carboxymyglobin kept at different relative humidity (RH) environments, showed variations in their spectra in the Soret bad region. For the samples which were kept at low hydration (Bellow about 33% RH) the spectrum was characteristic of carboxy derivative, whereas at high hydration (above about 93% RH) the spectrum was characteristic of oxy derivative, and in the the intermediate region the spectrum was a mixture of both derivatives. This ligand change observed at high hydration, may be explained assuming that the protein has flexibility, and reach a conformational state which enables the ligand to GO in and out. At low hydrations the protein structure is rigid and such that the access to the heme group is closed becoming impossible the ligand change. This explanation agrees with several experimental results that point to the existence of two structures to these hemoproteins in solution

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No presente trabalho, realizado com hemoproteínas na forma de pó, o efeito da hidratação foi observado através de espectroscopia fotoacústica. Amostras de carboxi-hemoglobina e carboxi-mioglobina mantidas em diferentes ambientes de umidade relativa (UR), mostraram variações em seus espectros na região da banda de Soret. Para amostras mantidas em baixa hidratação característico do derivado carboxi, em alta hidratação (acima de aproximadamente 90% UR) o espectro era característico do derivado carboxi e na região intermediária o espectro era de uma mistura dos dois derivados. Essa mudança de ligante observada em alta hidratação pode ser explicada supondo que a proteína tem flexibilidade e atinge um estado conformacional que possibilita a entrada e saída do ligante. Em baixa hidratação a estrutura da proteína é rígida e tal que o acesso ao grupo heme está fechado, impossibilitando a troca do ligante. Essa explicação é coerente com vários resultados experimentais que indicam a existência de duas estruturas para essas hemoproteínas em solução / At the present work accomplished with powder of hemoproteins, the hydration effect was observed through photoacoustic spectroscopy. Samples of caroxyhemoglobin and carboxymyglobin kept at different relative humidity (RH) environments, showed variations in their spectra in the Soret bad region. For the samples which were kept at low hydration (Bellow about 33% RH) the spectrum was characteristic of carboxy derivative, whereas at high hydration (above about 93% RH) the spectrum was characteristic of oxy derivative, and in the the intermediate region the spectrum was a mixture of both derivatives. This ligand change observed at high hydration, may be explained assuming that the protein has flexibility, and reach a conformational state which enables the ligand to GO in and out. At low hydrations the protein structure is rigid and such that the access to the heme group is closed becoming impossible the ligand change. This explanation agrees with several experimental results that point to the existence of two structures to these hemoproteins in solution

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A espectroscopia fotoacústica e de fluorescência foram empregadas no estudo de reação da transferência de elétrons entre um doador (Octaetil-porfirina) dois tipos de aceitadores [Diclorodiciano-benzoquinona (DDQ) e Duroquinona (DQ)] em um meio rígido [poli (metil-metacrilato)] . Foram preparados filmes nos quais a concentração de doador foi mantida constante e a de aceitador foi variada. Observou-se um aumento exponencial da amplitude do sinal fotoacústico do doador em 620 nm, com o aumento da concentração de aceitadores nos filmes. O modelo de Perrin para a supressão de fluorescência foi aplicado aos dados de fotoacústica e o raio da esfera de ação, que representa a distância crítica para a ocorrência da transferência de elétrons, foi determinado. Os resultados obtidos foram: para DDQ37 angstron e para aDQ 32 a 34angstron. Era esperado um raio maior para a DDQ devido a sua maior elétron afinidade. Também foi aplicado a estes dados o modelo de Kaneko, desenvolvido para a supressão de fluorescência. Dele se obtém a distribuição de moléculas aceitadoras incorporadas na esfera de ação. Para uma mesma concentração de aceitadores (2,8mmoldm-3) , a probabilidade de encontrar uma molécula de DDQ na esfera de ação foi 27%, enquanto que a probabilidade de encontrar uma molécula de DQ na esferade ação foi de 20%. Este resultado é, na verdade, equivalente ao encontrado no modelo de Perrin pois a probabilidade maior encontrada para a DDQ vem do fato do raio da sua esfera de ação ser maior. O valor encontrado para o raio crítico com os dados de fluorescência foi de 34 A para a DQ. Isto demonstra que as duas técnicas são complementares e que a espectroscopia fotoacústica pode ser usada para monitorar o processo de transferência de elétrons / Steady-state photoacoustic and fluorescence spectroscopy were employed to study the electron-transfer reaction from donor molecules (Octaethyl-porphirin) to two types of acceptor molecules [Dichloro-dicyano-benzoquinone (DDQ) and Duroquinone (DQ)I in a rigid medium [poly (methyl -metacrylate)] . Films were prepared with a fixed donor concentration and severa1 acceptor concentrations. It was observed an exponential growth in the donor photoacoustic signal amplitude at 620 nm, with the increase in the acceptor concentration. Perrin model, used in fluorescence quenching, was applied to the photoacoustic data and the radius o£ an action sphere, which represents a critica1 distance for the electron transfer process, was determined. The results obtained were: for DDQ 37 angstron and for DQ from 32 to 34 angstron. It was expected a larger radius for DDQ than for DQ due to its stronger electron affinity. Kaneko\'s model, was also applied to these data. It provides the distribution o£ incorporated acceptor molecules in the action sphere. For the same acceptor concentration (2.8 mmol , the probability of finding one DDQ molecule in the action sphere was 27%, while for the DQ molecule this value was 20%. Actually, this result is equivalent to that found using Perrin model, because the larger probability obtained for DDQ comes frm the fact that its critical radius is bigger . The value obtained for the critica1 radius from the fluorescence data was 34 angstron for DQ. This shows that these two techniques are complementary and that photoacoustic spectroscopy can be used to monitor the electron transfer process

A transferência de elétrons tem sido objeto de um estudo intenso nos últimos anos, por causa da importância deste tipo de reação em processos naturais como a fotossíntese. Com isto, um progresso considerável foi conseguido na proposição de modelos para o centro de reação fotossintético, em particular utilizando o sistema-modelo porfirina-quinona. Nosso intuito e estudar o processo de transferência de elétrons da porfirina para a quinona, aleatoriamente distribuídas em uma matriz polimérica, utilizando a técnica de espectroscopia fotoacústica. A utilização de um filme de polímero como meio tem duas vantagens. A primeira e aproximar nosso sistema-modelo do processo fotossintético natural, no qual os doadores e os aceitadores de elétrons estão envoltos nas proteínas do centro de reação e, portanto, em um meio polimérico. A segunda e possibilitar a utilização desses filmes como possíveis componentes eletrônicos moleculares. Identificamos os estados eletrônicos da porfirina e da quinona e tentamos determinar o estado de cargas separadas, P+ e Q-. A partir dos espectros obtidos, determinamos a eficiência quântica de fluorescência da porfirina utilizada nos filmes. Estudamos, também, a degradação da porfirina nos filmes preparados. Por fim, verificamos o efeito da concentração crescente da quinona nos filmes preparados com a porfirina / The electron transfer phenomenon has been the subject of intense study for the last years, due to the importance of this kind of reaction in natural processes as photosynthesis. A great improvement has been achieved in the proposition of models for the photosynthetic reaction center, in particular using the porphyrin-quinone model system. Our intention is to study the electron transfer process of the porphyrin to the quinone randomly distributed in a polymeric matrix, using the photo acoustic spectroscopy. The utilization of a polymeric film as an environment has two advantages. The first is to approximate our model system to the natural photosynthetic process, in which the electron donors and acceptors are surrounded by, the proteins of the reaction center, and thus in a polymeric environment. The second is to allow the utilization of these films as possible molecular electronic components. We identified the electronic states of the porphyrin and the quinone, and we attempted to determine the charge separated electronic state. We determined the fluorescence quantum efficiency of the porphyrin films, by their photo acoustic and absorption spectra. Also, we studied the degradation of the porphyrin in the prepared films. Finally, we checked the effect of the increasing concentration of the quinone in the films prepared with the porphyrin

During the last few years the scientific interest in chalcogenides glasses has been provoked on account of their properties and new application possibilities. These materials exhibit electrical and optical properties, which make them useful for several potential applications. Specifically the threshold and memory switching behavior and the infrared transmission of many of these glasses make the materials to be well suitable for use in memory devices and in fiber optics. Multicomponent glasses have been found to be more useful for many of these applications since the properties could be tailored for the specific uses. On account of this there has been great deal of interest in recent years in understanding the composition dependent variations of physical properties in these glasses. Models based on network topology and chemical ordering have been proposed to explain the composition dependence of physical properties. The Chemically Ordered Covalent Network (COCN) model is one of the best efforts put forth in this subject. This model predicts distinctive physical properties of these glasses for compositions at which there is a maximum number of heteropolar bonds. A physical model based on changes in network topology with composition has been proposed recently. This model predicts the rigidity to percolate in the network at the mean coordination number <r> = 2.40. This critical value of <r> at which the rigidity percolates is called the mechanical threshold or the rigidity percolation threshold. One more argument based on medium range interactions, existing in these glassy networks, suggests that the mechanical threshold should occur at <r> = 2.67. A general lack of consensus in the existing experimental reports on the mechanical threshold in some chalcogenides glasses prevents one from identifying the correct threshold value of <r>. A systematic study of the composition dependence of glasses with a large glass-forming region is necessary to resolve this controversy. The correct threshold value of <r> and the reason for the departure from this value in the other cases is the first step towards verifying the applicability of this model to chalcogenide glasses. Glasses belonging to IV — V — VI groups are natural candidates for this study because of their large glass forming region. It also seems possible to isolate the chemical threshold from interfering with the mechanical threshold in some of these glasses. In device applications of any semiconductor the optical and the electrical band gaps need to be varied and this is commonly done by doping. The large density of valence alteration pairs and intrinsic disorder of amorphous semiconductors counter-balances the effects of external additives. As a result, it is hard to electrically dope these materials. Non-equilibrium experimental techniques have been used to some extent, but one of the limitations is that they are confined to the thin film state. The finding that p to n type conduction sign changes can be induced by Bi and Pb in bulk Ge-M (M= S, Se and Te) glasses has therefore created special interest. This thesis deals with Ge-Se glass matrix doped with Te, Bi and Pb. The optical, thermal and electrical properties have been studied. The present thesis work is arranged in several chapters. The basic introduction of chalcogenide glasses is given in chapter one. This includes an introduction to chalcogenide glasses followed by a brief discussion on the important structural models, the possible defects in chalcogenide glasses and the electrical, optical and thermal properties of chalcogenide glasses. The second chapter discusses the experimental techniques used in the present investigations. The basic principles and theory behind the experiments, the experimental setup and the experimental procedure leading to the determination of the physical properties are given here. These include information about Differential Scanning Calorimetry (DSC), Photo acoustic (PA) spectroscopy and Photoluminescence studies. In the third chapter the experimental investigations on Ge-Se-Te glasses are presented. The chapter starts with the preparation and characterization of these glasses. It then gives an account of the earlier studies on Ge-Se-Te glasses that are relevant to the present work. The results of the DSC and PA studies are discussed in the following two sections. In the systems with Gex Se80-x Te20 and Gex Se75.x Te25, glasses with less than 20 at. % of Ge do not show any crystallization peak due to Se rich content. But Te and Ge-rich glasses show strong crystallization tendency. The composition dependence of Tg of this glassy system gives an evidence for the occurrence of the topological threshold or mechanical threshold at <r> = 2.40 and chemical threshold at <r> = 2.67. These can be explained on the basis of COCN model. The optical band gap and thermal diffusivity studies also show anomalous behavior at <r> = 2.40 and <r> = 2.67. The experimental results on Ge-Se-Te glasses are summarized in the last section of this chapter. The investigations on Bi doped Ge-Se and Ge-Se-Te glasses are given in the fourth chapter. The chapter starts with a brief introduction of preparation, characterization and a short review of earlier work. In PA studies the anomalous behavior is observed in thermal diffusivity and thermal diffusion length plot at 8-9 at. % of Bi doping of the Ge-Se and Ge-Se-Te glasses where the conduction changes from p to n type. These results are explained on the basis of percolation model and the formation of Bi2Se3 microcrystalline phase. Finally these results are summarized at the end of the chapter. The fifth chapter is devoted to the investigations on Pb doped Ge-Se glasses. It is arranged in five sections; preparation and characterization, earlier work, Photo acoustic and Photoluminescence studies. In PA studies the composition dependence of thermal diffusivity show anomalous behavior at x =F 9 at % of Pb in Pbx Ge42-x Sesg glasses and y = 21 at. % of Ge in Pb2o Gey Seso-y glasses where the conduction changes from p to n type. After that it reaches the maximum. After the conduction sign changes the conductivity increases with addition of respective Pb and Ge concentration in both series of glasses, which is reflected in thermal diffusivity value also. The results have been explained on the basis of COCN model. From PL studies, the PL intensity is high in un-doped Ge42 Scss glasses. With the addition of Pb into Ge-Se system the PL intensity goes down drastically up to 9 at. % of Pb, beyond 9 at. % the PL intensity is approximately the same up to 15 at. %. In the last section the results are summarized. Chapter six summarizes the essential features of the work reported in the thesis. These conclusions are drawn from the present and the earlier reported studies on Ge-Se-Te glasses, Bi doped Ge-Se and Ge-Se-Te glasses and Pb doped Ge-Se glasses. Finally based on the present experimental results, some future work has been suggested which could throw some light on a better understanding of/? to n transition and defects state of these glasses. It is worth extending the microscopic phase separation studies in these glasses. Highly sensitive experimental techniques are needed in this regard. Also some simulation work like Monte-Carlo simulation and Molecular dynamics simulation needs to be undertaken for understanding the microscopic phase separation and the role of defects in carrier type reversal in these glassy materials. All the references cited in the thesis are collected and listed at the end of the thesis.

A transferência de elétrons tem sido objeto de um estudo intenso nos últimos anos, por causa da importância deste tipo de reação em processos naturais como a fotossíntese. Com isto, um progresso considerável foi conseguido na proposição de modelos para o centro de reação fotossintético, em particular utilizando o sistema-modelo porfirina-quinona. Nosso intuito e estudar o processo de transferência de elétrons da porfirina para a quinona, aleatoriamente distribuídas em uma matriz polimérica, utilizando a técnica de espectroscopia fotoacústica. A utilização de um filme de polímero como meio tem duas vantagens. A primeira e aproximar nosso sistema-modelo do processo fotossintético natural, no qual os doadores e os aceitadores de elétrons estão envoltos nas proteínas do centro de reação e, portanto, em um meio polimérico. A segunda e possibilitar a utilização desses filmes como possíveis componentes eletrônicos moleculares. Identificamos os estados eletrônicos da porfirina e da quinona e tentamos determinar o estado de cargas separadas, P+ e Q-. A partir dos espectros obtidos, determinamos a eficiência quântica de fluorescência da porfirina utilizada nos filmes. Estudamos, também, a degradação da porfirina nos filmes preparados. Por fim, verificamos o efeito da concentração crescente da quinona nos filmes preparados com a porfirina / The electron transfer phenomenon has been the subject of intense study for the last years, due to the importance of this kind of reaction in natural processes as photosynthesis. A great improvement has been achieved in the proposition of models for the photosynthetic reaction center, in particular using the porphyrin-quinone model system. Our intention is to study the electron transfer process of the porphyrin to the quinone randomly distributed in a polymeric matrix, using the photo acoustic spectroscopy. The utilization of a polymeric film as an environment has two advantages. The first is to approximate our model system to the natural photosynthetic process, in which the electron donors and acceptors are surrounded by, the proteins of the reaction center, and thus in a polymeric environment. The second is to allow the utilization of these films as possible molecular electronic components. We identified the electronic states of the porphyrin and the quinone, and we attempted to determine the charge separated electronic state. We determined the fluorescence quantum efficiency of the porphyrin films, by their photo acoustic and absorption spectra. Also, we studied the degradation of the porphyrin in the prepared films. Finally, we checked the effect of the increasing concentration of the quinone in the films prepared with the porphyrin

A espectroscopia fotoacústica e de fluorescência foram empregadas no estudo de reação da transferência de elétrons entre um doador (Octaetil-porfirina) dois tipos de aceitadores [Diclorodiciano-benzoquinona (DDQ) e Duroquinona (DQ)] em um meio rígido [poli (metil-metacrilato)] . Foram preparados filmes nos quais a concentração de doador foi mantida constante e a de aceitador foi variada. Observou-se um aumento exponencial da amplitude do sinal fotoacústico do doador em 620 nm, com o aumento da concentração de aceitadores nos filmes. O modelo de Perrin para a supressão de fluorescência foi aplicado aos dados de fotoacústica e o raio da esfera de ação, que representa a distância crítica para a ocorrência da transferência de elétrons, foi determinado. Os resultados obtidos foram: para DDQ37 angstron e para aDQ 32 a 34angstron. Era esperado um raio maior para a DDQ devido a sua maior elétron afinidade. Também foi aplicado a estes dados o modelo de Kaneko, desenvolvido para a supressão de fluorescência. Dele se obtém a distribuição de moléculas aceitadoras incorporadas na esfera de ação. Para uma mesma concentração de aceitadores (2,8mmoldm-3) , a probabilidade de encontrar uma molécula de DDQ na esfera de ação foi 27%, enquanto que a probabilidade de encontrar uma molécula de DQ na esferade ação foi de 20%. Este resultado é, na verdade, equivalente ao encontrado no modelo de Perrin pois a probabilidade maior encontrada para a DDQ vem do fato do raio da sua esfera de ação ser maior. O valor encontrado para o raio crítico com os dados de fluorescência foi de 34 A para a DQ. Isto demonstra que as duas técnicas são complementares e que a espectroscopia fotoacústica pode ser usada para monitorar o processo de transferência de elétrons / Steady-state photoacoustic and fluorescence spectroscopy were employed to study the electron-transfer reaction from donor molecules (Octaethyl-porphirin) to two types of acceptor molecules [Dichloro-dicyano-benzoquinone (DDQ) and Duroquinone (DQ)I in a rigid medium [poly (methyl -metacrylate)] . Films were prepared with a fixed donor concentration and severa1 acceptor concentrations. It was observed an exponential growth in the donor photoacoustic signal amplitude at 620 nm, with the increase in the acceptor concentration. Perrin model, used in fluorescence quenching, was applied to the photoacoustic data and the radius o£ an action sphere, which represents a critica1 distance for the electron transfer process, was determined. The results obtained were: for DDQ 37 angstron and for DQ from 32 to 34 angstron. It was expected a larger radius for DDQ than for DQ due to its stronger electron affinity. Kaneko\'s model, was also applied to these data. It provides the distribution o£ incorporated acceptor molecules in the action sphere. For the same acceptor concentration (2.8 mmol , the probability of finding one DDQ molecule in the action sphere was 27%, while for the DQ molecule this value was 20%. Actually, this result is equivalent to that found using Perrin model, because the larger probability obtained for DDQ comes frm the fact that its critical radius is bigger . The value obtained for the critica1 radius from the fluorescence data was 34 angstron for DQ. This shows that these two techniques are complementary and that photoacoustic spectroscopy can be used to monitor the electron transfer process

The aim of the thesis is to study mechanical properties of nanomaterials (multi-layer graphene, silicon, mica) suitable to be used as novel pressure sensors in laser photoacoustic spectroscopy. Membranes (diameter ~ 4 mm, thickness ~ 100 nm) were prepared by mechanical exfoliation method and then attached to a glass window in several slightly different designs. Movement of these membranes was detected using HeNe laser beam reflected from the membrane's surface onto a position sensitive detector. Methanol was used as a model gas and the signal was collected from studied element and microphone simultaneously. Acoustic wave, induced inside a measuring cell by periodic thermal variations, causes the membranes to move. The movement of a membrane is influenced by its mechanical properties, which is possible to determine by fitting the measured data into a mathematical model. Comparison of the output data of all membranes' measurements shows, that the signal intensity is influenced by the method of attaching membrane to a glass window and by volume of free space on a side of a membrane. Metallization of the membrane's surface (~ 70 nm) decreases its springiness thus decreases the sensitivity. Several membranes reached sensitivity comparable with top class microphone.