A novel UHV microcalorimeter has been used to study the interaction between calcium and three polymers: MEH-PPV, MEH-PPP and P3HT. All three polymers behave differently in their reaction kinetics with calcium. On MEH-PPV we measure 45 μJ/cm² of heat generated in excess of the heat of bulk metal growth, 120 μJ/cm² for MEH-PPP, and 100 μJ/cm² for P3HT. Comparison of the MEH-PPV and MEHPPP data indicate that the initial reaction of calcium with MEH-PPV occurs at the vinylene group. We propose, based on hypothetical models, that calcium reacts with the vinylene groups of MEH-PPV with a reaction heat of 360 kJ/mol and at a projected surface density of 1.7 sites/nm², while it reacts with the phenylene groups of MEH-PPP in a two-step process with reaction heats of 200 and 360 kJ/mol respectively, at a projected surface density of 3.5 sites/nm². Optical absorption experiments, using either a 1.85 eV diode laser or a xenon lamp coupled to a scanning monochromator, have also been performed using the same calorimeter sensor. In the case of MEH-PPV, using the laser we find an optical absorption cross-section of 3E-¹⁷ cm² per incident calcium atom at low coverages. The change in absorptance at higher coverages correlates perfectly with the population of reacted Ca atoms determined calorimetrically. The size of the absorbance cross-section, and its position just within the band gap of the polymer, are consistent with the reaction being one of polaron formation. Calcium does not appear to dope P3HT, while the photon energy range of 1.5 to 3.75 eV used in these experiments is likely too small for probing polaronic energy states in MEH-PPP.

Utilizando a Dinâmica Molecular Tight Binding (TBMD), parametrizada para sistemas de carbono e hidrogênio, simulamos com condições periódicas de contorno e modelos de fatia, superfícies de diamante (100) puras e hidrogenadas em modelos de reconstruções ideais usualmente presentes na literatura, analisando o seu comportamento geométrico e eletrônico. Em seguida abordamos o comportamento morfológico e eletrônico, em simulações com temperaturas que variam entre 100K e 2000K de dois modelos de superfícies monohidrogenadas, que apresentam dois domínios em torno de uma estrutura de depressão local, característica de filmes de alta rugosidade. Em oposição à grande estabilidade térmica exibida pelo modelo monohidrogenado ideal e pelas colunas contínuas de dímeros, os modelos com depressão apresentaram significativa migração de átomos de hidrogênio para regiões subsuperficiais. Em nossas simulações os átomos de hidrogênio ficaram confinados nas regiões subsuperficiais, introduzindo uma desordem morfológica na superfície e nas regiões internas à fatia, induzindo estados eletrônicos nesta região, que levam ao fechamento do gap, passando a caracterizar uma fase quase-metálica. / By using the Tight Binding Molecular Dynamics (TBMD), parametrized to describe carbon and hydrogen atoms composed of systems, we apply periodic boundary conditions, slab models in order to simulate (100) clean and hydrogenated diamond surfaces. We study first the standard models used in the literature, analyzing their geometrical and eletronic behavior. We then focus on the morphological and electronic properties, in simulations under finite temperature dynamics ranging from 100K up to 2000K, of two distinct models of monohydride surfaces; Each model exhibits two distincts domains in the surface pattern characterized by a local depression, characteristic of rough surfaces. In opposition to the high thermal stability observed for ideal monohydrogenated surfaces and the extended dimer rows, these models showed an expressive hydrogen migration to the subsurface regions. In our simulations the hydrogen atoms remain in the subsurface regions, but introduce morphological disorder at the surface and in the slab internal regions. These hydrogen atoms induce electronic states mostly localized in the subsurface region, which are responsible for closing the gap, and leading the system to exhibit a quasi-metallic phase.

A espectroscopia foto-térmica tem sido largamente usada na investigação de propriedades térmicas e ópticas de materiais sólidos. Neste trabalho, desenvolvemos novas câmaras foto-térmicas as quais foram adaptadas para os estudos de materiais poliméricos. Estendemos o modelo desenvolvido por Mandelis para a espectroscopia fotopiroelétrica (PPES), incluindo nele um termo devido à reflexão de luz na interface amostra-detetor. A aplicação da técnica PPES em filmes de Poli(3-Butiltiofeno) não dopado nos permitiu obter sua condutividade e difusividade térmicas, como também seu gap de energia. Também aplicamos a técnica fotoacústica, com um flash de laser He-Ne, ao estudo de filmes de polímeros transparentes. Finalmente, desenvolvemos um método semi-empírico o qual significa a análise do sinal foto-térmico, quando ele é, principalmente, devido à difusão térmica. / Photothermal spectroscopies have been largely used in the investigation of thermal and optical properties of solids materials. In this work we developed new photothermal cells which were adapted for the study of polymerics materials. We also extended the model developed by Mandelis for the Photopyroeletric Spectroscopy (PPES), including in it a term due to the reflected light in the sample-detector interface. The application of the PPES technique in films of undopedpoly(3-butylthiophene) allowed us to obtain its thermal conductivity and diffusivity, as well as its gap energy. We also applied the photoacoustic technique, with a flash of He-Ne laser to study of transparent films of polymers. Finally we developed a semi-empiric method which simplifies the analysis of the photothermal signal, when it is mainly due to the thermal diffusion.

Utilizando a Teoria do Funcional da Densidade junto com o formalismo do pseudopotencial de primeiros princípios, realizamos um estudo sistemático do processo de adsorção da molécula de oxigênio sobre a superfície livre de CdTe (110) nas reconstruções 1x1, 1x2 e 2x1. Este estudo consistiu na determinação das adsorções energeticamente favoráveis e na viabilidade de suas formações através da análise das barreiras de ativação. Nossas análises indicam que apenas uma molécula de oxigênio adsorve sobre a superfície livre em uma reconstrução 1x1 e que não ocorre a quebra da molécula durante o processo de adsorção. As estruturas formadas foram divididas nos regimes de baixas e altas temperaturas. Do estudo das barreiras de ativação verificamos que no regime de baixas temperaturas a molécula de oxigênio liga-se exclusivamente ao Cd da primeira camada através de ligações Cd-O-O ou Cd-O2. A configuração da superfície de CdTe com a molécula adsorvida, se assemelha a configuração do cristal. As estruturas de faixas de energia neste regime apresentam um estado característico de defeito duplo aceitador. Para o regime de altas temperaturas, a molécula adsorve entre o Cd da primeira camada e o Te da segunda camada, quebrando esta ligação Cd-Te e também quebrando a ligação que o Cd da segunda camada realiza com o Te da terceira camada. O complexo formado apresenta ligações Cd-O, Cd-O2, Te-O e O-O e as estruturas de faixas de energia apresentam um gap indireto entre os pontos gama e X de 1.30 eV. / Density Functional Theory with first-principles pseudopotential formalism have been used to a systematic research of the oxygen molecule adsorption on the free surface of CdTe(110) in the 1x1, 1x2 and 2x1 reconstructions. This research was based on the determination of the adsorptions energetically favorables and the viability of each formation through their activation barriers analysis. This analysis indicates that only one oxygen molecule adsorbs over the free surface of the CdTe(110) in the 1x1 reconstruction and that the dissociation of the molecule does not occur during the adsorption process. The structures were divided on the high and low temperature regimes. From the activation barriers study it was verified that on the regime of low temperatures the oxygen molecule bind exclusively to the Cd of the first layer through the Cd-O-O or Cd-O$_2$ bonds. The CdTe surface configuration with the adsorbed molecule looks like a crystal configuration. The energy band structure, on this regime, shows a characteristic state of double acceptor defect. For the high temperature regime the molecule adsorbs between the Cd of the first layer and the Te of second layer, breaking the Cd-Te bond between them and also breaking the bonds that the Cd of the second layer does with the third layer. The complex shows Cd-O, Cd-O2, Te-O and O-O bonds and the energy band structure shows an indirect gap between the gamma and X points of 1.30eV.

This diploma thesis discusses the gas sensor preparation via anodic oxidation. It names sensor types, deals with the sensing principle of electrochemical sensors in detail and submits sensor parameters. It describes preparation technology and characterization technology methods. In the experimental part, it focuses on both the measurement methodology and the electrochemical oxygen sensor covered with titanium dioxide nanocolumns fabrication. Not the least it discusses acquired research results.

A novel UHV microcalorimeter has been used to study the interaction between calcium and three polymers: MEH-PPV, MEH-PPP and P3HT. All three polymers behave differently in their reaction kinetics with calcium. On MEH-PPV we measure 45 μJ/cm² of heat generated in excess of the heat of bulk metal growth, 120 μJ/cm² for MEH-PPP, and 100 μJ/cm² for P3HT. Comparison of the MEH-PPV and MEHPPP data indicate that the initial reaction of calcium with MEH-PPV occurs at the vinylene group. We propose, based on hypothetical models, that calcium reacts with the vinylene groups of MEH-PPV with a reaction heat of 360 kJ/mol and at a projected surface density of 1.7 sites/nm², while it reacts with the phenylene groups of MEH-PPP in a two-step process with reaction heats of 200 and 360 kJ/mol respectively, at a projected surface density of 3.5 sites/nm². Optical absorption experiments, using either a 1.85 eV diode laser or a xenon lamp coupled to a scanning monochromator, have also been performed using the same calorimeter sensor. In the case of MEH-PPV, using the laser we find an optical absorption cross-section of 3E-¹⁷ cm² per incident calcium atom at low coverages. The change in absorptance at higher coverages correlates perfectly with the population of reacted Ca atoms determined calorimetrically. The size of the absorbance cross-section, and its position just within the band gap of the polymer, are consistent with the reaction being one of polaron formation. Calcium does not appear to dope P3HT, while the photon energy range of 1.5 to 3.75 eV used in these experiments is likely too small for probing polaronic energy states in MEH-PPP. / Science, Faculty of / Chemistry, Department of / Graduate

Les matériaux thermoélectriques sont des matériaux capables de convertir l’énergie thermique en énergie électrique en exploitant l’effet Seebeck et vice-versa, en exploitant l’effet Peltier. Grâce à ces deux effets, il est possible de récupérer l’énergie perdue sous forme de chaleur dans la plupart des activités humaines (industrie, automobile,…) ou bien de produire du froid de manière efficace et silencieuse. Pour une efficacité optimale, il faut se tourner vers des matériaux qui possèdent simultanément une faible résistivité électrique, (rhô), une faible conductivité thermique (lambda) et un fort pouvoir thermoélectrique (ou coefficient Seebeck alpha). En d’autre termes, on peut monter que le facteur a optimiser est le facteur de mérite ZT = alpha2.T/rhô.lambda (une valeur de ZT de 1 est considérée comme élevée). Les verres de chalcogénures, grâce à leurs structures désordonnées, présentent naturellement un lambda bas mais sont trop résistifs (à l’opposé des matériaux thermoélectriques classiques dont on cherche à diminuer la conductivité thermique). Dans ce travail, deux stratégies ont été mises en places afin d’abaisser la résistivité électrique et d’augmenter ainsi les performances thermoélectriques des verres de chalcogénures. En nous focalisant sur les verres de tellurures, nous avons d’abord cherché à modifier leur composition et ajouter des éléments métalliques tels que Cu. La substitution de Te par Se dans le système Cu-As-Te a également permis d’augmenter la stabilité en température. Finalement pour des matériaux vitreux, un ZT maximum de l’ordre de 0,1 a été obtenu à 375K, pour le composé Cu30As10Te54Se6.La seconde solution consiste en une vitrocéramisation de ces verres : en profitant du mélange de matériau vitreux et de matériau cristallin, il est possible de tirer parti des propriétés de chacun (respectivement une conductivité thermique basse et un résistivité électrique basse) et d’augmenter le facteur ZT. En optimisant les vitrocéramiques de la composition Cu15As30Te55, nous avons pu obtenir un ZT proche de 0,2 à 375K. L’évolution des propriétés en fonction de la fraction cristalline et de la microstructure n’est toutefois pas facile à prédire, ce qui nous a également mené à la mise en place d’un modèle de transport dans les composites biphasés, donnant quelques indications sur les directions à suivre pour finalement améliorer ces matériaux davantage / Thermoelectrics are materials capable of converting thermal energy into electrical energy through Seebeck effect, and vice-versa through Peltier effect. By using these two phenomena, it becomes possible to salvage heat loss from most human activities (industries, cars,…) or on the other side, to efficiently and silently produce cold. To obtain an efficient material, it is necessary to look for materials that simultaneously possess a low electrical resistivity, a low thermal conductivity and a high thermoelectric power alpha (or Seebeck coefficient). In other words, it is possible to show that we need to optimize the figure of merit ZT = alpha2.T/rho.lambda (a ZT as high as 1 can be considered as efficient). Chalcogenide glasses, due to favorably disordered structures, exhibit a naturally low thermal conductivity, but have a too high electrical resistivity (oppositely to classical thermoelectrics of which we seek to lower the thermal conductivity). In this work, two strategies were set up into lowering electrical resistivity and then further enhance the thermoelectric performance of chalcogenide glasses. Focusing on telluride glasses, we firstly tried to modify their composition and add metallic elements such as copper. Substituting Te par Se in the ternary system Cu-As-Te allowed increasing their thermal stability. For vitreous materials, we finally obtained a maximal ZT around 0.1 at 375K, for the compound Cu30As10Te54Se6. The second solution consists in partially crystallizing these glasses: by taking advantage of the favorable properties of each phase (the low thermal conductivity of the glassy phase and the low electrical resistivity of the crystalline phase), the figure of merit can be raised. By optimizing glass-ceramics of composition Cu15As30Te55, a ZT close to 0.2 at 375K has been obtained. However, predicting how the thermoelectric properties evolve with crystalline fraction or microstructure is complex. That led us to set up a transport model for two-phases composites, giving finally some insights to further improve these materials.

This diploma thesis discusses the gas sensor preparation via anodic oxidation. It names sensor types, deals with the sensing principle of electrochemical sensors in detail and submits sensor parameters. It describes preparation technology and characterization technology methods. In the experimental part, it focuses on both the measurement methodology and the electrochemical oxygen sensor covered with titanium dioxide nanocolumns fabrication. Not the least it discusses acquired research results.

<p><a>Molecular imaging revolutionized the way researchers and clinicians visualize and investigate complex biochemical phenomena, and it is beneficial </a><a>for disease diagnosis, drug design and therapy assessment</a>. Among a variety of different imaging techniques, the non-ionizing and non-invasive photoacoustic (PA) imaging is attracting increased attentions, owing to its high spatial and temporal resolutions with reasonable penetration depth in tissue. Parallel efforts have been the preparation of PA imaging agents which has high PA efficacy and can specifically label the targets at cellular or molecular level. Particularly, there is exponentially growing interest in imaging in the second near-infrared (NIR-II) window (1000–1700 nm), where offers reduced tissue background and improved penetration depth. However, study of PA imaging in the NIR-II window is incomplete, partly due to the lack of suitable materials. Therefore, in my dissertation work I studied NIR-II PA imaging through semiconducting polymer. </p> <p>Firstly, the performance of PA imaging in the NIR-II window is explored by using a semiconducting polymer nanoparticle (SPN) which has strong absorption in the NIR-II window. Compared with lipid, blood and water, such SPN shows outstanding PA contrast in the NIR-II window <i>in situ</i> and <i>in vivo</i>, and an imaging depth of more than 5 cm at 1064 nm excitation is achieved in chicken-breast tissue. These results suggest that SPN as a PA contrast in the NIR-II window opens new opportunities for biomedical imaging with improved imaging contrast and centimeter-deep imaging depth.</p> <p>Next, targeted PA imaging of prostate cancer is achieved by functionalizing a NIR-II absorbing SPN with prostate-specific membrane antigen (PSMA)-targeted ligands. Insights into the interaction of the imaging probes with the biological targets are obtained from single-cell to whole-organ by transient absorption (TA) microscopy and PA imaging. TA microscopy reveals the targeting efficiency, kinetics, and specificity of the functionalized SPN to PSMA-positive prostate cancer at cellular level. Meanwhile, the functionalized SPN demonstrates selective accumulation and retention in the PSMA-positive tumor after intravenous administration <i>in vivo</i>. Taken together, it is demonstrated that BTII-DUPA SPN is a promising targeted probe for prostate cancer diagnosis by PA imaging. </p> <p>Lastly, PA imaging in the NIR-II window is also achieved water-soluble semiconducting polymer, which is prepared by oxygen-doping. After doping, it shows broadband absorption in the entire NIR-II window, with great chemical stability, photostability and biocompatibility. Owing to its merit of broadband absorption, the imaging depth comparison among different NIR-II wavelengths is also achieved. Moreover, this doped semiconducting polymer is readily soluble in normal physiological pH by virtue of carboxyl groups on side chains and tends to aggregate at an acidic environment which results in a 7.6-fold PA enhancement at pH 5.0. Importantly, a 3.4±1.0-fold greater signal in tumor tissue than that in muscle is revealed <i>in vivo</i>. This study provides a more attainable yet effective platform to the field for achieving water-soluble NIR-II absorbing contrast agents for activatable PA imaging. </p>

Conjugated polymers are very attractive materials for the scientists and industry due to low cost of the organic compounds, their lightweight, easy large-area processing from solution at low temperature and mechanical flexibility. Moreover, these materials are multifunctional and advanced technologies require both simultaneous n- and p-type conductance, i.e. ambipolarity. However, there are some hindrances which do not allow the wide spreading of this new generation of semiconductors into the market, first of all, due to their instability to ambient conditions. Moreover, determination of the tunable parameters which are responsible for high efficiency and controlled crystal packing ordering of the devices is rather complicated. A lot of efforts are done in order to improve the performance of the organic electronics as well as to shed light on the relation between the chemical structure and their intrinsic properties. Additionally, the governing factors which define the conductive properties of these materials are still under debate and this remains a great challenge for the researchers. One way to gain insight into the characteristics of polymeric materials is to begin exploring the polymers from their small constitutive units and then step-by-step to construct and characterize every compound up to macromolecular level. In this work, the semiconducting block copolymers, as promising candidates for application in organic transistors, are investigated starting from their small donor and acceptor blocks up to monomers and macromolecules, using computational methods running on different time and length scales. It is found out that the charge transport depends on the symmetry of molecules and the hopping mobilities can be predicted from isolated stacks of dimers, which are defined by minimum energy, without knowledge of the actual crystal structure. Interestingly, the polymers moieties prefer to build up mixed stacks and the flanks form segregated columns if there are no present defects in the samples. At each step of the investigation the results are compared with available experimental data.