Savitvarkiai monosluoksniai suteikia metalų paviršiams norimas savybes ir plačiai taikomi elektronų pernašos tyrimuose, konstruojant (bio)jutiklius, biotechnologinius bei fotoelektroninius procesus. Teigiamo krūvio monosluoksniai naudojami kuriant anijonų jutiklius ir (bio)technologinius procesus su adsorbuotomis neigiamo krūvio makromolekulėmis. Darbe buvo susintetinta bifunkcinė molekulė su galinėmis tiolio ir piridinio grupėmis, suformuotas monosluoksnis ir ištirtos jo struktūrinės ir funkcinės savybės. Pagrindiniai darbo tikslai buvo ištirti N-(6-merkapto)heksilpiridinio (MHP) adsorbuoto ant Au ir Ag elektrodų struktūrą ir nustatyti monosluoksnio sąveikos su neorganiniais anijonais, dodecilsulfato anijonu ir grafeno oksidu dėsningumus. Naudojant paviršiaus sustiprintos Ramano spektroskopijos, kvantų chemijos skaičiavimo ir izotopinio pakeitimo metodus nustatyti MHP struktūros ir orientacijos elektrodo atžvilgiu Ramano sklaidos žymenys. Tiriant juostų intensyvumo priklausomybes nuo potencialo ir žadinančios spinduliuotės bangos ilgio parodyta, kad Au/MHP sistemoje pasireiškia krūvio pernešimo Ramano spektrų stiprinimo mechanizmas. Nustatyta, kad adsorbuotų neorganinių anijonų pilnai simetrinio virpesio dažnis sumažėja lyginant su tirpalo spektru ir tas pokytis koreliuoja su Gibso dehidracijos energija. Parodyta, kad MHP pritraukia grafeno oksidą. Nustatyta, kad grafeno oksido C-C ryšio ilgis ir elektroninė struktūra gali būti keičiama, keičiant potencialą. / Self-assembled monolayers provide possibility of changing metal surface properties in controllable manner and are widely used in studies of electron transfer, construction of (bio)sensors, and biotechnological and photoelectronic processes. Positively charged monolayers are valuable in development of sensors for anions and (bio)technological processes with adsorbed negatively charged macromolecules. In this work the structural and functional properties of monolayer formed from synthesized molecule with terminal thiol and pyridinium groups have been studied. The main tasks were to assess the structure of N-(6-mercapto)hexylpyridinium (MHP) on Ag and Au electrodes, and to determine the peculiarities of interaction with inorganic anions, dodecylsulfate, and graphene oxide. Based on surface enhanced Raman spectroscopy (SERS), quantum chemical calculations, and isotopic substitution studies, the Raman marker bands for structure and orientation of MHP have been evaluated. Dependence of SERS intensity on potential and excitation wavelength has revealed the operation of charge transfer Raman enhancement mechanism. It was found that the frequency of symmetric stretching mode of adsorbed ions decreases comparing with solution value and the extent of the shift correlates with the Gibbs dehydration energy. Adsorption of graphene oxide at MHP monolayer has been demonstrated. The electronic structure and length of C-C bonds of graphene oxide was found to be altered by the potential.

Self-assembled monolayers provide possibility of changing metal surface properties in controllable manner and are widely used in studies of electron transfer, construction of (bio)sensors, and biotechnological and photoelectronic processes. Positively charged monolayers are valuable in development of sensors for anions and (bio)technological processes with adsorbed negatively charged macromolecules. In this work the structural and functional properties of monolayer formed from synthesized molecule with terminal thiol and pyridinium groups have been studied. The main tasks were to assess the structure of N-(6-mercapto)hexylpyridinium (MHP) on Ag and Au electrodes, and to determine the peculiarities of interaction with inorganic anions, dodecylsulfate, and graphene oxide. Based on surface enhanced Raman spectroscopy (SERS), quantum chemical calculations, and isotopic substitution studies, the Raman marker bands for structure and orientation of MHP have been evaluated. Dependence of SERS intensity on potential and excitation wavelength has revealed the operation of charge transfer Raman enhancement mechanism. It was found that the frequency of symmetric stretching mode of adsorbed ions decreases comparing with solution value and the extent of the shift correlates with the Gibbs dehydration energy. Adsorption of graphene oxide at MHP monolayer has been demonstrated. The electronic structure and length of C-C bonds of graphene oxide was found to be altered by the potential. / Savitvarkiai monosluoksniai suteikia metalų paviršiams norimas savybes ir plačiai taikomi elektronų pernašos tyrimuose, konstruojant (bio)jutiklius, biotechnologinius bei fotoelektroninius procesus. Teigiamo krūvio monosluoksniai naudojami kuriant anijonų jutiklius ir (bio)technologinius procesus su adsorbuotomis neigiamo krūvio makromolekulėmis. Darbe buvo susintetinta bifunkcinė molekulė su galinėmis tiolio ir piridinio grupėmis, suformuotas monosluoksnis ir ištirtos jo struktūrinės ir funkcinės savybės. Pagrindiniai darbo tikslai buvo ištirti N-(6-merkapto)heksilpiridinio (MHP) adsorbuoto ant Au ir Ag elektrodų struktūrą ir nustatyti monosluoksnio sąveikos su neorganiniais anijonais, dodecilsulfato anijonu ir grafeno oksidu dėsningumus. Naudojant paviršiaus sustiprintos Ramano spektroskopijos, kvantų chemijos skaičiavimo ir izotopinio pakeitimo metodus nustatyti MHP struktūros ir orientacijos elektrodo atžvilgiu Ramano sklaidos žymenys. Tiriant juostų intensyvumo priklausomybes nuo potencialo ir žadinančios spinduliuotės bangos ilgio parodyta, kad Au/MHP sistemoje pasireiškia krūvio pernešimo Ramano spektrų stiprinimo mechanizmas. Nustatyta, kad adsorbuotų neorganinių anijonų pilnai simetrinio virpesio dažnis sumažėja lyginant su tirpalo spektru ir tas pokytis koreliuoja su Gibso dehidracijos energija. Parodyta, kad MHP pritraukia grafeno oksidą. Nustatyta, kad grafeno oksido CC ryšio ilgis ir elektroninė struktūra gali būti keičiama, keičiant potencialą.

[pt] Estruturas baseadas em grafeno como óxido de grafeno (OG) e óxido de grafeno reduzido (OGr) vêm sendo amplamente utilizadas em aplicações de sensoriamento resistivo de gás. Entretanto, poucos projetos são efetuados utilizando métodos pervasivos e não intrusivos, que são importantes para aplicações onde intervenções podem ser problemáticas. Este trabalho apresenta a implementação de protótipos de sensores sem fio de baixo custo baseados na tecnologia de RFID sem chip, para sensoriamento de vapor de álcool, utilizando uma topologia de antena miniaturizada baseada em Metamateriais (MTMs) carregada com OGr. Simulações utilizando o método dos elementos finitos são efetuadas de forma a encontrar o melhor local para deposição das estruturas sensíveis ao vapor de álcool. É observado que a estrutura responde a variações de resistividade de OGr apenas para uma determinada faixa de valores. O tempo de redução térmica de OG necessário para atingir este espectro de valores é experimentalmente determinado, estando entre 60 e 90 min à 200 Graus Celsius. Amostras de GO são fabricadas utilizando o método de Hummer modificado, e são depositadas nos gaps das antenas. Posteriormente, são reduzidas por 60, 75 e 90 minutos. O setup de medição consistiu em medições do coeficiente de reflexão em banda X. Após um determinado tempo para estabilização, álcool isopropílico e também etanol são colocados em contato com a amostra em um recipiente fechado por 1h30, e a resposta foi observada. Resultados com sensibilidade de até 11,5 por cento foram obtidos. / [en] Graphene oxide (GO) and reduced graphene oxide (rGO) based structures have been widely applied for resistive gas sensing applications. However, few projects are developed using pervasive and non-intrusive methods, which are important for applications where intervention can be an issue. This work presents the implementation of low-cost wireless sensor prototypes based on chipless RFID technology, for alcohol vapor sensing, by using a metamaterial (MTM) based miniaturized antenna loaded with rGO. Simulations are performed using finite element method in order to find the best place to deposit the alcohol vapor sensitive structures. It is observed that the structure responds to resistivity variations only for a determined range of values. The GO reduction time necessary to reach this spectrum of values is experimentally determined, and it is found to be between 60 and 90 min at 200 Celsius degrees. GO samples are synthesized using a modified Hummer s method, and deposited in the gaps of the antenna structures. Later, they are reduced for 60, 75 and 90 min. The measurement setup consists in reflection coefficient characterization at X band frequencies. After a stabilization time, isopropyl alcohol and ethanol are put in contact with the samples in a closed container for 1h30, and the response is observed. Sensitivities up to 11,5 percent are obtained.

Magister Scientiae - MSc / The toxicity of microcystin is associated with the inhibition of serine/threonine protein phosphatases 1 and 2A, which can lead to hepatocyte necrosis and haemorrhage. Analysis of microcystin is most commonly carried out using reversed-phase high performance liquid chromatographic methods (HPLC) combined with ultra-violet (UV) detection .The ability of these techniques to identify unknown microcystin in environmental samples is also restricted by the lack of standard reference materials for the toxins. Highly specific recognition molecules such as antibodies and molecularly imprinted polymers (MIPs) have been employed in the pre-concentration of trace levels of microcystin from water and show great potential for the clean-up of complex samples for subsequent analysis. New biosensor technologies are also becoming available, with sufficient sensitivity and specificity to enable rapid ‗on-site‘ screening without the need for sample processing. In this work we constructed a Protein phosphatase biosensor for detection of microcystin-LR in aqueous medium, onto polyamic acid/graphene oxide (PAA: GO) composite electrochemically synthesised in our laboratory. The composites were synthesised at three different ratios i.e. 50:50, 80:20 and 20:80 to evaluate the effect of each component in the search to produce highly conductive mediator platforms. The electrochemistries of the three different composites were evaluated using CV and SWV to study interfacial kinetics of the materials as thin films at the glassy carbon electrode. The phosphatase biosensor parameters were evaluated using CV, SWV, EIS and Uv-vis spectroscopy. The affinity binding of the microcystin-LR to protein phosphatase 2A was investigated using electrochemical impedance spectroscopy which is a highly sensitive method for measuring interfacial kinetics of biosensor systems.

A galvanic cell converts chemical energy into electrical energy. Devices that carry out these conversions are called batteries. In batteries, generally the chemical components are contained within the device itself. If the reactants are supplied from an external source as they are consumed, the device is called a fuel cell. A fuel cell converts chemical energy into electrical energy as long as the chemicals are supplied from external reserves. The working principle of a metal-air battery involves the principles of both batteries and fuel cells. The anode of a metal-air cell is stored inside the cell, whereas O2 for the air-electrode is supplied from either atmosphere or a tank. There are several metal-air batteries available academically, which include Zn-air, Alair, Fe-air, Mg-air, Ca-air, Li-air and Na-air batteries. So far, only Zn-air battery is successfully commercialized. Li-air battery is attractive compared to other metal-air batteries because of its high theoretical energy density (11140 Wh kg-1). The energy density of Li-air battery is 3 - 5 times greater than state-of-art Li-ion battery. Li-air (or Li-O2) battery comprises Li-metal as the anode and a porous cathode. The cathode and the anode are separated by a suitable separator soaked in an organic electrolyte. Atmospheric air can enter the battery through the porous cathode. Out of the mixture of gases present in the air, only O2 is electrochemically active. For optimization purpose, most of researchers use pure O2 gas instead of air. Li-air battery is not commercialized till now because of several issues associated with it. The issues include: (i) sluggish kinetics of O2 electrode reaction, (ii) decomposition of the electrolyte during charge-discharge cycling, (iii) formation of Li dendrites, (iv) contamination by moisture, etc. Among these scientific and technical problems related to Li-O2 cell system, studies on rechargeable O2 electrode with fast kinetics of oxygen reduction reaction (ORR) during the cell discharge and oxygen evolution reaction (OER) during charge in non-aqueous electrolytes are important. In non-aqueous electrolytes, the 1-electron reduction of O2 to form superoxide (O2 -) is known to occur as the first step. (ii) Subsequently, superoxide undergoes reduction to peroxide (O2 2-) and then to oxide (O2-). The kinetics of ORR is slow in non-aqueous electrolytes. Furthermore, the reaction needs to be reversible for rechargeable Li-air batteries. In order to realize fast kinetics, a suitable catalyst is essential. The catalyst should be bifunctional for both of ORR and OER in rechargeable battery applications. Noble metal particles have been rarely investigated as catalysts for O2 electrode of Li-O2 cells. Graphene has two-dimensional planar structure with sp2 bonded carbon atoms. It has become an important electrode material owing to its high electronic conductivity and large surface area. It has been investigated for applications such as supercapacitors, Li-ion batteries, and fuel cells. Catalyst nanoparticles prepared and anchored to graphene sheets are expected to sustain discrete existence without undergoing agglomeration and therefore they possess a high catalytic stability for long term experiments as well as applications. In this context, it is intended to explore the catalytic activity of noble metal nanoparticles dispersed on reduced graphene oxide (RGO) for O2 electrode of Li-O2 cells. While a majority of the investigations reported in the thesis involves noble metal and alloy particles dispersed on RGO sheets, results on polypyrrole-RGO composite and also magnesium cobalt silicate for Li-O2 system are included. A chapter on electrochemical impedance analysis of LiMn2O4, a cathode material of Li-ion batteries, is also presented in the thesis. Introduction on electrochemical energy storage systems, in particular on Li-O2 system is provided in the 1st Chapter of the thesis. Synthesis of Ag nanoparticles anchored to RGO and catalytic activity are presented in the 2nd Chapter. Ag-RGO is prepared by insitu reduction of Ag+ ions and graphene oxide in aqueous phase by ethylene glycol as the reducing agent. The product is characterized by powder XRD, UV-VIS, IR, Raman, AFM, XPS, SEM and TEM studies. The SEM images show the layered morphology of graphene and TEM images confirm the presence of Ag nanoparticles of average diameter less than 5 nm anchored to RGO (Fig. 1a). Ag-RGO is investigated for ORR in alkaline (1 M KOH), neutral (1 M K2SO4) and non-aqueous 0.1 M tetrabutyl ammonium perchlorate in dimethyl sulphoxide (TBAP-DMSO) electrolytes. The ORR follows 4e- reduction in aqueous and 1e- reduction pathway in non-aqueous electrolytes. Li-O2 cells are assembled with Ag-RGO as (iii) Fig. 1. (a) TEM image of Ag-RGO and (b) charge-discharge voltage profiles of Li-O2 (Ag-RGO) cells. oxygen electrode catalyst in non-aqueous electrolyte (1 M LiPF6-DMSO) and subjected to charge-discharge cycling at several current densities. The discharge capacity values obtained are 11950 (11.29), 9340 (5.00), and 2780 mAh g-1 (2.47 mAh cm-2) when discharged at 0.2, 0.5, 0.8 mA cm-2, respectively (Fig. 1b). Powder XRD studies of discharged electrodes indicate the formation of Li2O2 and Li2O during the cell discharge. In addition to these studies, Na-O2 cells are also assembled with Ag-RGO in non-aqueous electrolyte. It is concluded that the chemistry Li-O2 and Na-O2 cells are similar except for the capacity values. Metal nanoparticles of Au, Pd and Ir are decorated on RGO sheets by reduction of metal ions on graphene oxide by NaBH4. Au-RGO, Pd-RGO and Ir-RGO are characterized by various physicochemical techniques. Particle size of metal nanoparticles ranges from 2 to Fig.2. Charge-discharge voltage profiles Li-O2(RGO) (i) and Li-O2(Au-RGO) (ii) cells at current density 0.3 mA cm-2. 0 2500 5000 7500 10000 12500 15000 10 nm on graphene sheets. All samples are studied for ORR in aqueous and non-aqueous electrolytes by cyclic voltammetry and rotating disk electrode experiments. Li-O2 cells are assembled in 1 M LiPF6-DMSO and discharge capacity values obtained are 3344, 8192 and 11449 mAh g-1 with Au-RGO, Pd-RGO and Ir-RGO, respectively, at 0.2 mA cm-2 current density. The results of these studies are described in Chapter 3. Synthesis and electrochemical activity of Pt-based alloy nanoparticles (Pt3Ni, Pt3Co and Pt3Fe) on RGO are presented in Chapter 4. The Pt3Ni alloy particles are prepared by simultaneous reduction of Pt4+, Ni2+ and graphene oxide by hydrazine in ethylene glycol medium. Pt3Co-RGO and Pt3Fe-RGO are also prepared similar to Pt3Ni-RGO. Formation of alloys is confirmed with XRD studies. O2 reduction reaction on Pt-alloys in non-aqueous electrolyte follows 1e- reduction to O2 -. RDE results show that Pt3Ni-RGO is a better catalyst than Pt for O2 reduction (Fig. 3). Li-O2 cells are assembled with all samples and subjected to Fig. 3. Linear sweep voltammograms of Pt3Ni-RGO, Pt3Co-RGO and Pt3Fe-RGO in 0.1 M TBAPDMSO with 1600 rpm at 10 mV s-1 scan rate. The area of GC electrode was 0.0314 cm2 with a catalyst mass of 200 μg. charge-discharge cycling at several current densities. The initial discharge capacity values obtained are 14128, 5000 and 10500 mAh g-1 with Pt3Ni-RGO, Pt3Co-RGO and Pt3Fe-RGO, respectively, as the air electrode catalysts. Polypyrrole (PPY) is an attractive conducting polymer with advantages such as high electronic conductivity and electrochemical stability. A combination of advantages of graphene and PPY composite are explained in the Chapter 5. PPY is grown on already synthesized RGO sheets by oxidative polymerization of pyrrole in an acidic PY composite is characterized by XRD and Raman spectroscopy studies. Li-O2 cells are assembled in non-aqueous electrolyte and subjected for charge-discharge cycling at different current densities. The discharge capacity value of Li-O2(PPY-RGO) cell is 3358 mAh g-1 Fig. 4. (a) Discharge-charge performance of Li-O2(PPY-RGO) cell with a current density of 0.2 mA cm-2 limiting to a capacity of 1000 mAh g-1 and (b) variation of cut-off voltages on cycling. (3.94 mAh cm-2) in the first cycle. Li-O2(PPY-RGO) cell delivers 3.7 times greater discharge capacity than Li-O2(RGO) cell. Cycling stability of Li-O2 (PPY-RGO) cell is investigated by charge-discharge cycling by limiting the capacity to 1000 mAh g-1, and the cell voltage at the end of discharge and at the end of charge are found constant at 2.75 and 4.10 V, respectively (Fig. 4 a, b). This study shows that PPY-RGO is stable in Li-O2 cells. Electrochemical impedance study shows that charge-transfer resistant is 500 Ω for freshly assembled Li- O2(PPY-RGO) cell and it decreases to 200 Ω after 1st discharge. Synthesis of magnesium cobalt silicate and its electrochemical activity are presented in Chapter 6. MgCoSiO4 is synthesized by mixed solvothermal approach and characterized by various physicochemical techniques. Cubic shaped MgCoSiO4 is investigated for oxygen evolution reaction (OER) activity in alkaline and neutral media. The current values at 0.95 versus SHE are 43, 0.18, 16 mA cm-2 on MgCoSiO4, bare carbon paper and Pt foil electrodes, respectively (Fig. 5), indicating that MgCoSiO4 is a good catalyst for OER. The onset potential for OER is 0.68 V versus SHE on MgCoSiO4 in 1 M KOH. OER activity on MgCoSiO4 is also studied in K2SO4 and phosphate buffer electrolytes. The results indicate good catalytic activity of MgCoSiO4 in neutral electrolytes also. The catalytic activity of Fig. 5. Cyclic voltammograms of bare carbon paper (i), Pt foil (ii), MgCoSiO4 coated carbon (iii) electrodes in 1 M KOH (sweep rate = 5 mV s-1, loading level = 1.15 mg, area = 0.5 cm-2). MgCoSiO4 towards ORR in aqueous and non-aqueous electrolytes is studied by RDE experiments. Li-O2 cells are assembled with bifunctional MgCoSiO4 catalyst in 1 M LiPF6- DMSO electrolyte and the discharge capacity values obtained are 7721 (8.27), 2510 (1.66) and 1053 mAh g-1 (0.92 mAh cm-2) when discharged at 0.3, 0.5 and 0.8 mA cm-2 current densities, respectively. Electrochemical impedance spectroscopy (EIS) measurements of LiMn2O4 electrode are carried out at different temperatures from -10 to 50 0C and in the potential range from 3.50 to 4.30 V, and the data are analysed in Chapter 7. In the EIS spectra recorded over the frequency range from 100 kHz to 0.01 Hz at different temperatures, there are two semicircles present in the Nyquist plot (Fig. 6a). But in 3.90 to 4.10 V versus Li/Li+(1M) potential range at low temperatures (-10 to 15 oC) range, another semicircle also appears (Fig. 6b). Impedance parameters such as solution resistant (Rs), charge-transfer resistance (Rct), doublelayer capacitance (Cdl), electronic resistance (Re) and Warburg impedance (WR), etc., are obtained by analysis of the EIS data. The variations of resistances with temperature are analysed by Arrhenius-like relationships and the apparent activation energies of the corresponding transport properties are evaluated. The values of activation energy for chargetransfer process are 0.37, 0.30 and 0.42 eV, at 3.50, 3.90 and 4.10 V versus Li/Li+(1M), respectively. The chemical diffusion coefficient of Li+ ions into LiMn2O4 calculated from EIS data. The values of diffusion coefficient calculated are in the range of 2.50 x 10-12 - 4.10 Fig. 6. Nyquist plot of impedance study of Li/LiMn2O4 cell at 3.50 V (a) and 3.90 V (b) at -10 0C. Details of the above studies are described in the thesis.

Les liquides ioniques et le graphène sont intensivement étudiés, respectivement en tant qu’électrolyte et électrode, pour le développement des supercondensateurs. Dans ce cadre, il est primordial de caractériser l’interface entre les deux espèces. Pour ce faire, nous avons réalisé ce type d’interface par la procédure des films de Langmuir que nous avons observés à différentes échelles via des mesures d’isothermes, de microscopies à angle de Brewster et à force atomique ainsi que par diffusion des rayons X de surface. Nous avons étudié des films formés par des liquides ioniques, de l’oxyde de graphène et enfin d’un mélange de ces deux espèces. L’étude sur les liquides ioniques purs montre que le cation joue un rôle non négligeable sur l’organisation des films à l’interface air-eau, aussi bien en monocouche que lors du passage en phase tridimensionnelle. Par ailleurs, nous avons montré que les films d’oxyde de graphène forment spontanément une bicouche de feuillets à l’interface eau-air même pour de faibles densités superficielles. Enfin concernant les films mixtes, nous avons observé une ségrégation verticale des espèces quand la pression de surface devient suffisamment élevée. Le film est alors composé d’une première couche en contact avec l'eau, majoritairement composée de feuillets d’oxyde de graphène parallèles à l’interface, sur laquelle se superpose une seconde couche formée des domaines de liquide ionique désorganisé. / Graphene and ionic liquids are intensively studied, respectively as electrolyte and as electrode materials, for the development of supercapacitors. In this framework, the characterization between the two species is essential. We realized such kind of interfaces through the Langmuir film procedure and characterized them at different scales, using isotherm measurements, Brewster Angle and Atomic Force Microscopies, and surface X-ray scattering. We studied films formed by different ionic liquids, by graphene oxide and finally by a mixture of the two species. The study on the pure ionic liquids evidences the role of the cation on the film organization at the air-water interface, for the monolayer as well as for the tridimensional phase. Moreover, we showed that the graphene oxide films are composed of a bilayer of sheets à the interface, even at low surface densities. Finally, regarding the mixed film, we observed a vertical segregation of the species for high enough surface pressures. The film is formed by a first layer in contact with the water surface, mostly composed of graphene oxide sheets parallel to the interface, on which a second layer is superimposed, composed of disorganized ionic liquid domains.

CAPES - Coordenação de Aperfeiçoamento de Pessoal de Nível Superior / CNPq - Conselho Nacional de Desenvolvimento Científico e Tecnológico / FAPEMIG - Fundação de Amparo a Pesquisa do Estado de Minas Gerais / Na presente tese foram desenvolvidas três plataformas para a construção de biossensores visando o diagnóstico molecular da hepatite C, hepatite B e artrite reumatoide, por técnicas eletroquímicas, ópticas e microscópicas, usando amostras reais. Os genossensores para hepatites C e B foram desenvolvidos sobre a superfície de um eletrodo de ouro modificado com nanomateriais, sendo esses o óxido de grafeno e o óxido de grafeno reduzido, respectivamente. Em todos os biossensores propostos a interação da sonda com o alvo foi efetivamente verificada pelas diferentes técnicas. No caso do genossensor para hepatite C, o óxido de grafeno foi modificado quimicamente com etilenodiamina e apresentou limites de detecção e quantificação de 1:483 (v/v) e 1:145 (v/v), respectivamente, usando amostras de soro de pacientes positivos. A interação da sonda específica do HCV: gRNA causou uma redução na amplitude de resposta de corrente de cerca de 2,9 vezes quando comparada ao controle negativo, usando a VPD. O genossensor para a hepatite B a sonda foi imobilizada sobre eletrodo de ouro contendo óxido de grafeno reduzido, ouro descoberto e nanoparticulas de ouro. A análise usando VPD indica que a adição de DNA genômico de HBV provocou um aumento de cerca de 1,4 vezes na amplitude de corrente de pico quando comparado ao controle negativo. Em adição, análises de SPR mostraram que as amostras positivas de HBV resultaram em uma alteração de cerca de 15 vezes em comparação com as amostras negativas. No biossensor desenvolvido para o diagnóstico da artrite reumatoide foi utilizado um eletrodo de grafite modificado com um filme poli(3-hidroxibenzóico), no qual foi imobilizado um peptídeo mimético que reconhece o anticorpo anti-CAIII. O sensor mimético desenvolvido permitiu a distinção entre amostras positivas e negativas para a artrite reumatóide, uma vez que apresentou uma diminuição expressiva no sinal de corrente de cerca de 2,2 vezes, quando comparado ao soro negativo. Assim, foi possível desenvolver plataformas analíticas, seletivas e específicas fornecendo novas abordagens para o diagnóstico clínico e aplicações point-of-care para o monitoramento de doenças inflamatórias e infecciosas. / In the present thesis, three biosensing platforms aiming the molecular diagnosis of hepatitis C, hepatitis B and rheumatoid arthritis were developed by electrochemical, optical and microscopic techniques using real samples. The genosensors for the diagnosis of hepatitis C and B were developed on a gold electrode modified with nanomaterials, being these graphene oxide and reduced graphene oxide, respectively. In all proposed biosensors the interaction of the probe with the target was effectively verified by the different techniques. In the case of the genossensor for hepatitis C, graphene oxide was chemically modified with ethylenediamine and showed limits of detection and quantification of 1:483 (v/v) and 1:145 (v/v), respectively, using serum samples from positive patients. The interaction of the HCV probe and the gRNA caused a reduction in current response amplitude of about 2.9 fold as compared to the negative control, using the DPV. The genossensor for hepatitis B probe was immobilized on a gold electrode containing reduced graphene oxide, gold disks and gold nanoparticles. Analysis using DPV indicates that the addition of HBV gDNA caused an increase of about 1.4 times in peak current amplitude, when compared to the negative control. In addition, SPR analyzes showed that positive samples of HBV resulted in a change of about 15- fold compared to negative samples. In the biosensor developed for the diagnosis of rheumatoid arthritis, a graphite electrode modified with a poly (3-hydroxybenzoic) film was used, in which a mimetic peptide that recognizes the anti-CAIII antibody was immobilized. The developed mimetic sensor allowed the distinction between positive and negative samples for rheumatoid arthritis, since it presented an decrease in the current signal of about 2.2 times, when compared to the negative serum. Thus, it was possible to develop analytical, selective and specific platforms, providing new approaches for clinical diagnosis and point-of-care applications, for the monitoring of inflammatory and infectious diseases. / Tese (Doutorado)

The motivation of this thesis is to understand the physical properties of semiconductor quantum dots (QDs) and to get insight on the basic physics of charge separation in composites made from QDs with graphene oxide (GO)/organic semiconductors. The flexion phonon interactions is one of fundamental issues in solid state physics, which has a significant effect on both electrical and optical properties of solid state materials. This thesis investigates the physical properties of aqueous grown QDs through exciton-phonon coupling and non-radiative relaxation of excited carriers which have been carried out by temperature dependent photoluminescence spectroscopy. Several e orts have been made in order to understand the basic physics of photo induced charge separation in the hybrid systems made from QDs with graphene oxide and organic semiconductors. Investigations on the photoconductivity of the devices made from these hybrid composites have been carried out keeping the motive of its application in nanotechnology. This thesis work is presented in six chapters inclusive of summary and directions for future work. Chapter 1 discusses the background knowledge and information of the general properties of semiconductor nanostructures, QDs and their hybrid nanocomposites. Chapter 2 deals with the sample preparation and experimental techniques used in this thesis. Chapter 3 elaborates the exciton-phonon scattering and nonradiative relaxations of excited carriers in visible emitting cadmium telluride QDs with help of temperature and size dependent photoluminescence. Chapter 4 presents the investigations on time resolved photoluminescence dynamics and temperature dependent photoluminescence properties of near infrared (NIR) emitting mercury cadmium telluride (CdHgTe). Chapter 5 discusses the importance of NIR emitting silver sulphide (Ag2S) QDs and gives insight of nonradiative recombinations through defect/trap states. Chapter 6 investigates the excited state interactions between CdHgTe QDs and GO. Chapter 7 focuses on the understanding of basic physics of charge separation/transfer between poly (3hexylthiophene) and Ag2S QDs. Chapter 1: Semiconductor nanostructures have attracted significant scientific attention due to their fundamental physical properties and technological interests. Quasi zero dimensional nanocrystals or quantum dots (QDs) have shown unique optical and electrical properties compared to its bulk counterpart. These QDs show discrete energy levels due to the quantum confinement effect hence known as arti cial atoms. Large surface to volume ratio in these QDs is expected to play a crucial role in determing the photo-physical properties. Temperature dependent photoluminescence is a powerful tool for understanding the role of the large surface area on exciton recombination process in QDs. Inorganic QDs combined with different materials like graphene oxide or organic semiconductors forms an exciting class of synthetic materials which integrates the properties of organic and inorganic semiconductors. It is quite important to understand the basic physics of electronic interactions in these composites for its future application in many elds. Chapter 2: Synthesis of the inorganic QDs, graphene oxide, composites and fabrication of devices is an important and integral part of this thesis. Hydrothermal and three necked ask technique is adopted to get highly dispersible colloidal quantum dots in solvents. Synthesis of graphene oxide from graphite through oxidation and ultrasonication has been carried out to obtain homogenous dispersed graphene oxide in water. Structural properties have been studied by techniques like X ray diffraction, Raman spectroscopy, X ray photoelectron spectroscopy and high resolution transmission electron microscopy. Morphological properties are studied by atomic force microscopy and transmission electron microscopy. Optical properties are investigated by absorption spectroscopy, steady state and time resolved photoluminescence spectroscopy. Photoconductivity characteristics are analyzed to understand the basics of enhanced current in the various devices made from QDs composites. Chapter 3:Investigations on exciton phonon coupling and nonradiative relaxations in various sizes of visible light emitting cadmium telluride (CdTe) QDs size have been presented. Due to the large surface area, QDs are prone to have defect/trap states which can affect the exciton relaxation. Hence, understanding the role of such defect/trap states on photoluminescence is very essential for achieving the optimum optical properties. Temperature dependent (15 300 K) photoluminescence has been used to understand nonradiative relaxation of excited carriers. Thermally activated processes and multiple phonons scattering is thoroughly investigated to understand the quenching of photoluminescence with temperature. The strength of exciton-phonon coupling is investigated which determines the variation in energy bandgap of QDs with temperature. Role of exciton phonon scattering is also discussed to understand the basic physics of photoluminescence line width broadening in QDs. Chapter 4 and 5: This part of thesis focuses on the size and temperature pho-toluminescence properties of near infra red emitting ternary alloyed CdHgTe and Ag2S QDs. Near infrared emitting semiconductor quantum dots (QDs) have attracted significant scientific and technological interests due to their potential applications in the fields of photosensor, solar energy harvesting cells, telecommunication and biological tissue imaging etc. Structural and photophysical properties of CdHgTe QDs have been analyzed by high resolution transmission electron microscopy, X rayphotoelectron microscopy, photoluminescence decay kinetics and low temperature photoluminescence. Investigations on the nonradiative recombinations through trap/defects states and exciton phonon coupling are carried out in colloidal Ag 2S QDs which emits in the range of 1065 1260 nm. Particularly, the photoluminescence quenching mechanism with increasing temperature is analyzed in the presence of multiple nonradiative relaxation channels, where the excited carriers are thermally stimulated to the surface defect/trap states of QDs. Chapter 6 and 7: The aim of these chapters is to understand the basic physics of photo induced charge separation in the hybrid systems made from the inorganic QDs with graphene oxide and organic semiconductors. In chapter 6, CdHgTe QDs are decorated on graphene oxide sheets through physisorption. The excited state electronic interactions have been studied by optical and electrical characterizations in these CdHgTe QDs GO hybrid systems. In chapter 7, investigations are carried out for understanding the basic physics of charge separation in the composites of Ag2S QDs and poly (3hexylthiophene 2,5 diyl)(P3HT). These composites of inorganic organic materials are made by simple mixing with help of ultrasonication technique. Steady state and time resolved photoluminescence measurements are used as powerful technique to gain insight of energy/charge transfer process between P3HT and Ag2S QDs. Furthermore, investigations have been carried out on the photoconductivity of the devices made from these hybrid composites keeping the motive of its application in nanotechnology. Chapter 8: The conclusions of the work presented in this thesis are coherently summarized in this chapter. Thoughts and prospective for future directions are also summed up.

Made available in DSpace on 2016-03-15T19:38:54Z (GMT). No. of bitstreams: 1 RODRIGO MENDES GEROSA.pdf: 6396087 bytes, checksum: b904e08a314dcda72a403496699b5206 (MD5) Previous issue date: 2015-08-26 / Fundo Mackenzie de Pesquisa / This thesis describes the development of new photonic devices produced by micromanipulation of the optical fibers properties, i.e., the change, in the micrometer scale, of the fiber s optical and/or geometrical properties. In this context, three lines of research have been followed, using different optical fiber processing techniques and considering different types of devices. In the first line, the coupling of two cores in a photonic crystal fiber with three initially uncoupled cores was demonstrated. The couplers had an insertion loss estimated at ~1 dB and exhibited spectral modulations with a depth up to 18 dB. They also showed high sensitivity to polarization, which can be exploited in fiber polarization beamsplitters. For this work, we used a technique that modifies the fiber structure by applying local differential pressure and heating. In the second line, a Rhodamine dye laser was develop with a fully fiber integrated optofluidic cavity. It was possible to maintain a high flow of the dye solution, up to 400 μL / min, which allowed the use of a pump laser with a high repetition rate (1 kHz), and, at the same time, the degradation of the gain medium was not observed. An optical conversion rate of up to 9% and a pump energy threshold lower than 1 mJ were obtained. A splicing technique was used, in which an angled cleaved capillary fiber was fused to a conventional fiber, thereby leaving a side inlet open for the fluid flow. The third line aimed at the incorporation of carbon nanomaterials to optical fibers. In this case, two approaches were employed: in one of them, polymeric films, with a thickness of 20 μm, containing carbon nanotubes were produced on the face of optical fiber patchcords; such patchcords have been inserted into erbium-doped fiber laser cavities to act as saturable absorbers in order to obtain mode-locking operation. Pulses with durations down to 364 fs were obtained with 10.2 nm bandwidths. The films were formed when a micro-droplet of a carbon nanotube suspension on an optical adhesive was placed on the surface of optical fiber connectors, with the use of a micropipette. Within the same line, photonic crystal fibers (PCFs) with homogeneous graphene oxide films covering the inner walls of their capillaries were obtained. The homogeneity was confirmed by Raman spectroscopy and by the loss per fiber length, as measured by the cut back method. A PCF was also spliced to conventional connectorized fiber patchcords and incorporated into a laser cavity to generate pulses. The film production was consisted of inserting a graphene oxide suspension into the PCF capillaries, after which the solvent was dried. / Essa tese descreve o desenvolvimento de novos dispositivos fotônicos produzidos a partir da micromanipulação das propriedades de fibras ópticas, isto é, da alteração em escala micrométrica, das propriedades ópticas e/ou geométricas destas. Nesse contexto, três linhas de trabalho foram seguidas, utilizando diferentes técnicas de processamento de fibras ópticas e levando à demonstração de diferentes tipos de dispositivos. Na primeira linha foi demostrado o acoplamento de dois núcleos em uma fibra de cristal fotônico com três núcleos inicialmente desacoplados. Os acopladores apresentaram uma perda de inserção estimada de ~1 dB e exibiram modulações espectrais com uma profundidade de até 18 dB. Apresentaram também uma sensibilidade elevada à polarização, que pode ser explorada em divisores de polarização (polarization beamsplitters) a fibra. Para isso foi utilizada uma técnica de alteração da estrutura da fibra através da aplicação de pressão diferencial e aquecimento local,. Na segunda linha foi desenvolvido um laser do corante Rodamina com uma cavidade optofluídica totalmente integrada em fibra. Nela, era possível manter um alto fluxo da solução de corante, de até 400 μl/min, o que permitiu utilizar um laser de bombeio com alta taxa de repetição (1kHz) sem observar-se degradação do meio de ganho. Uma taxa de conversão óptica de até 9% e uma energia de limiar (threshold) menor que 1 μJ foram obtidas. Utilizou-se aqui uma técnica de emenda através da qual uma fibra capilar clivada em ângulo era emendada com uma fibra convencional, deixando assim uma entrada lateral para fluidos. A terceira linha visou incorporar nanomateriais de carbono a fibras ópticas. Nesse caso duas abordagens foram empregadas: em uma, filmes poliméricos com espessuras de 20 μm e contendo nanotubos de carbono foram produzidos na face de conectores de cordões de fibra ópticas; esse cordões foram inseridos em cavidades laser a fibra dopada com érbio para atuar como absorvedores saturáveis para a obtenção de mode locking. Com isso foram obtidos pulsos de até 364 fs e espectros com larguras de banda de 10,2 nm. Os filmes foram formados a partir de uma microgota de uma suspensão de nanotubos de carbono em adesivos ópticos que foi colocada sobre a face de conectores de fibra óptica com uma micropipeta. Ainda na mesma linha obtiveram-se fibras de cristal fotônico (PCFs) com filmes de óxido de grafeno homogêneos no interior de seus capilares. A homogeneidade foi comprovada através de espectroscopia Raman e pela medida da perda em função do comprimento das fibras, realizada através do método cut back. Uma PCF foi, ainda, emendada a cordões de fibra convencional conectorizados e incorporada a cavidades laser para geração de pulsos. A produção dos filmes foi realizada através da inserção de uma suspensão de óxido de grafeno nos capilares de PCFs de núcleo sólido, após o qual o solvente era secado.

O objetivo desse trabalho foi desenvolver um compósito cerâmico de zircônia-grafeno para aplicação odontológica. Este estudo avaliou o efeito do pó de partida, concentração de grafeno e da temperatura de sinterização sobre as propriedades mecânicas (dureza e tenacidade à fratura) do compósito desenvolvido. Para isto foram sintetizados os pós de Y-TZP a partir de soluções de óxido-cloreto de zircônio e cloreto de ítrio na proporção desejada de 3mol% através da rota de co-precipitação em solução de hidróxido de amônio seguido por uma série de lavagens em água, etanol e butanol com posterior destilação azeotrópica, secagem, moagem e calcinação. O grafeno foi obtido a partir da exfoliação química de grafite pelo método de Hummers [40] modificado por Marcano [39], o que resultou em um gel acastanhado que foi submetido a lavagem por centrifugação, secagem e desaglomeração em almofariz de ágata, resultando, por fim, no óxido de grafeno. Uma segunda etapa foi o processo de redução química com ácido ascórbico para obtenção de óxido de grafeno reduzido, um pó de coloração escura que foi adicionado à Y-TZP para a obtenção do compósito nas diversas concentrações (em mol%) que foram estudadas: (0,01%, 0,05%, 0,10%, 0,50%, 1,00% e 2,00%). Os pós foram caracterizados por termogravimetria, difração de raios X e espectroscopia (FT-IR). Os espécimes foram confeccionados em matriz metálica cilíndrica e sinterizados em forno tubular em atmosfera inerte. Outros espécimes foram confeccionados em matriz de grafite de alta densidade e sinterizados por Spark Plasma Sintering (SPS). Todas as amostras foram caracterizadas por meio de ensaios de densidade, dureza Vickers, tenacidade à fratura e microscopia eletrônica de varredura. Os maiores valores de densidade relativa foram observados para as amostras sinterizadas em SPS, sendo que se obteve valor de densidade relativa de 98,7 % para a concentração de 0,50% de grafeno e 98,4% para a Y-TZP pura. Por outro lado, o maior valor encontrado em sinterização em atmosfera a 1400°C sem a presença de H2 para Y-TZP pura foi da ordem de 96,76%. Os valores de dureza foram maiores nas amostras sinterizadas em SPS, no entanto a tenacidade à fratura mostrou não se alterar em função do conteúdo de grafeno. As fotomicrografias de MEV mostraram que houve uma variação de tamanho de grão de acordo com a presença do grafeno e do método de sinterização. De acordo com os resultados obtidos neste trabalho foi possível concluir que o processamento desenvolvido permitiu a criação de um compósito cerâmico zircônia-grafeno que pôde ser caracterizado por diversos métodos analíticos. A densidade teórica do compósito desenvolvido não foi alcançada por meio de nenhum dos métodos de sinterização utilizados (Tubular ou SPS) e nem variando-se a temperatura. Para espécimes sinterizados em atmosfera inerte, a maior temperatura de sinterização (1400°C) e a presença do gás H2 não melhorou a densificação. Além disso, esses espécimes tiveram aumento da dureza com o aumento da concentração de grafeno, entretanto, a sua tenacidade à fratura não foi afetada pelo teor de grafeno. Para espécimes sinterizados por meio de SPS, a temperatura de sinterização de 1350°C resultou em melhores valores de densificação. Além disso, para este tipo de sinterização, tanto a dureza como a tenacidade à fratura foram afetadas pelo teor de grafeno. / The objective of this work was to develop a zirconia-graphene ceramic composite for dental application. The study evaluated the effect of the starting powder effect, graphene concentration and sintering temperature on the mechanical properties of the composite. For this, the Y-TZP powders were synthesized from zirconium chloride and yttrium chloride solutions in the desired ratio of 3 mol% through the co-precipitation route in ammonium hydroxide solution followed by a series of washes in water, ethanol and butanol with subsequent azeotropic distillation, drying, grinding and calcination. Graphene was obtained from the chemical exfoliation of graphite by the method of Humans modified by Marcano, which resulted in a brownish gel that was subjected to washing by centrifugation, drying and deagglomeration in agate mortar, resulting finally in the graphene oxide. A second step was the chemical reduction with ascorbic acid to obtain reduced graphene oxide, a dark-colored powder that was added to the Y-TZP to obtain the composite in the various concentrations (in mol%) that were studied (0, 01%, 0.05%, 0.10%, 0.50%, 1.00% and 2.00%). The powders were characterized by thermogravimetry, X-ray diffraction and spectroscopy (FT-IR). The specimens were made in cylindrical metallic matrix and sintered in a tubular oven. Other samples were made in high density graphite matrix and sintered by Spark Plasma Sintering (SPS). All samples were characterized by means of density tests, Vickers hardness, fracture toughness and scanning electron microscopy. The highest values of relative density were observed for the sintered samples in SPS. A relative density of 98.7% was obtained for the 0.50% concentration of graphene and 98.4% for the pure Y-TZP. On the other hand, the highest value found in tubular sintering at 1400 ° C without the presence of H2 for pure Y-TZP was of the order of 96.76%. The hardness values were higher in the sintered samples in SPS, however the fracture toughness showed not to change as a function of the content of graphene. SEM images showed that there was a variation of grain size according to the presence of graphene and the sintering method. According to the results of this study it was concluded that the process developed allowed the creation of a graphene-zirconia ceramic composite which can be characterized by various analytical methods. The theoretical density of the composite developed was not achieved by any of the sintering methods used (tubular or SPS) nor by varying the temperature. For tubular sintered specimens, the higher sintering temperature (1400 ° C) and the presence of H2 gas did not improve densification. In addition, these specimens had increased hardness with increasing graphene concentration, however, their fracture toughness was not affected by graphene content. For sintered specimens by SPS, the sintering temperature of 1350 ° C resulted in better densification values. In addition, for this type of sintering, both hardness and fracture toughness were affected by the content of graphene