Coordenação de Aperfeiçoamento de Pessoal de Nível Superior / Neste trabalho foi proposto o monitoramento do processo de cura e fotocura de resinas epóxi através da Espectroscopia Fotoacústica. Nos experimentos, foram utilizados dois tipos de resinas epóxi: A resina Epoxtec 331, com o endurecedor DER 24, e a resina fotocurada EBECRYL 3720-TP25, com o fotoiniciador OMNIRAD 808. Foram utilizados dois modelos de células fotoacústicas: uma baseada na técnica de diferença de fase dos dois feixes (T2F); e outra convencional. São apresentadas as montagens experimentais desenvolvidas para os monitoramentos da cura e fotocura das resinas. O estudo foi realizado monitorando o sinal fotoacústico fazendo varredura em comprimentos de onda. Também foi monitorado o sinal fotoacústico em função do tempo durante as curas e fotocuras. Foi estudado o efeito de luz saturante, não modulada, nos processos de fotocura. Tanto a amplitude quanto a fase do sinal fotoacústico revelaram-se boas ferramentas para o monitoramento proposto. Apesar de muitos dos efeitos encontrados, nos estudos realizados, ainda não terem explicação, o presente trabalho mostrou a potencialidade da espectroscopia fotoacústica para esta área de pesquisa. / In this work it was proposed the monitoring of the cure and photocuring of epoxy resins by Photoacoustic Spectroscopy. In the experiments, two types of epoxy resins were used: the resin Epoxtec 331,with the hardener DER 24; and the resin EBECRYL 3720 - TP25, with the photoinitiator 808 OMNIRAD. Two models of Photoacoustic cell were used: one based on two-beam phase-lag technique (T2F); and a conventional one. The developed set-ups for monitoring of cure and photocuring of epoxy resins are presented. The study was carried out with monitoring the photoacoustic signal on the wavelengths scan. Also the photoacoustic signal as a function of time was observed during the cure and photocuring. The effect of unmodulated saturating light was studied in the processes of photocuring. Both the amplitude and the phase of the photoacoustic signal proved to be good tools for the proposed monitoring. Although many of the effects found in these studies have not yet been explained, the present study showed the potential of photoacoustic spectroscopy to this area of research.

Orientador: Daniel Pereira / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Fisica Gleb Wataghin / Made available in DSpace on 2018-08-08T18:30:13Z (GMT). No. of bitstreams: 1 Costa_LeversonFariasLamonier_D.pdf: 15914858 bytes, checksum: 1c9b9d5747ffb493f5451d81d2898051 (MD5) Previous issue date: 2007 / Resumo: Neste trabalho realizamos três importantes etapas: 1) montar e caracterizar um laser selado de 13C02, 2) empregar o laser selado de 13C02 como fonte de bombeamento óptico para a molécula de metanol CH30H, e utilizá-lo pela primeira vez, para excitar o isótopo de metanol 13CH30H para geração de ondas na região do TeraHertz (THz) e 3) Propor "assignments" para as transições THz do CH30H e do 13CH30H. Para excitar as respectivas moléculas de metanol, um tubo comercial selado de 13C02 foi montado e caracterizado num ressonador laser Fabry-Perot. Dois cabeçotes de aluminio foram conectados por 4 barras de invar, separado em 135cm. Em um dos cabeçotes, temos uma grade de difração (150 linhas/mm) na configuração Littrow para selecionar as linhas de emissao do respectivo laser. 0 2° cabeçote suporta um espelho de saída de ZnSe (90% de refletividade com 10m de raio de curvatura) acoplado num PZT para sintonia fina da frequência do laser. No sistema de alimentação, usamos uma fonte de alta tensão comercial (25kV, 8mA) operando em regime DC. Com isso, utilizamos o respectivo laser para excitar as moléculas CH30H e 13CH30H, onde fomos pioneiro no uso do mesmo para bombeio óptico da molécula 13CH30H. Decorrente disso, obtemos os espectros de absorção em torno de cada linha de emissão do 13C02 dos respectivos metanol. Estes dados serviram de referenda para investigação sistemática de novas emissões THz, onde observamos e caracterizamos 12 novas linhas THz do CH30H e 19 do 13CH30H. Todas foram caracterizadas em relação ao seu comprimento de onda, offset, pressao de trabalho, polaridade e intensidade relativa.Utilizando os dados de linhas THz observados por nós, e os espectros de absorção a Transformada de Fourier do CH30H e do 13CH30H, um programa computacional intitulado "Ritz", identificou "assignments" para 4 transições THz do CH30H e 9 emissoes THz para 13CH30H, respectivamente / Abstract: In this work we accomplish three important tasks: to mount and to characterize a laser sealed-off 13C02 to optically pump first time methanol molecules CH30H and 13CH30H for generation of TeraHertz waves; Proposed assignments for transistions THz of the CH30H and 13CH30H. For optical pumping we use a commercial sealed-off 13C02, tube in a homemade Fabry-Perot laser resonator, mounted on two aluminum blocks connected by invar rods and separeted by 1.35m. One block holds a grating (150grooves/mm) used in Littrow configuration to select the emission line, while the second block supports a ZnSe output mirror (90% reflectivity and 10m radius of curvature) mounted on a PZT for fine frequency tuning. We use high voltage power supply (25kV, 8mA) to operate the 13C02 laser in CW regime. A cooling system maintains operation of the laser tube at -10o C. Output powers of l0 W and 1l0 MHz tuning range are typical for lines with higher optical gains. After, molecules CH30H and 13CH30H, optoacoustics spectroscopy (OA) signal, obtained around each sealed-off 13C02 laser line were the starting point to search for THz laser lines. For the more intense OA signal, a systematic investigation was performed to observe and characterize 12 new THz lines of the CH30H and 19 THz emissions of 13CH30H that they had been characterized in wavelength, offset, working pressure, relativepolarity and relative intensity. The available data has been compared a Ritz analysis of the high-resolution Fourier-Transform absorption spectrum of CH30H and 13CH30H, resulting in the assignments for 4 THz transistions of the CH30H and 9 THz emissions for 13CH30H, respectively / Doutorado / Física Atômica e Molecular / Doutor em Ciências

Submitted by Renata Lopes (renatasil82@gmail.com) on 2017-07-24T12:08:43Z No. of bitstreams: 1 alexandrepinheirodasilva.pdf: 29097377 bytes, checksum: 94bcde5f459e88c78cffbdf774e348a0 (MD5) / Approved for entry into archive by Adriana Oliveira (adriana.oliveira@ufjf.edu.br) on 2017-08-09T13:30:24Z (GMT) No. of bitstreams: 1 alexandrepinheirodasilva.pdf: 29097377 bytes, checksum: 94bcde5f459e88c78cffbdf774e348a0 (MD5) / Made available in DSpace on 2017-08-09T13:30:24Z (GMT). No. of bitstreams: 1 alexandrepinheirodasilva.pdf: 29097377 bytes, checksum: 94bcde5f459e88c78cffbdf774e348a0 (MD5) Previous issue date: 2011-09-30 / Neste trabalho vamos apresentar a implantação de duas técnicas fototérmicas: a fotoacústica de câmara aberta que possibilita encontrarmos a difusividade térmica dos materiais, e a técnica pc que fornece o valor do produto da densidade pelo calor específico da substância, conhecido como capacidade térmica volumétrica. Utilizamos também a técnica de lente térmica para a medida da difusividade térmica e do parâmetro dS/dT (taxa de variação do caminho óptico S). As técnicas mencionadas fornecem os parâmetros termo-ópticos (Difusividade Térmica, Condutividade Térmica e dS/dT ) para materiais vítreos como os vidros ferro fosfato, telurito, borossilicato e simulado lunar JSC-1. Modelos teóricos são apresentados e testados. Mostramos que o modelo da flexão termoelástica é dominante na maioria das amostras estudadas. Exceção foi observado no caso de vidros semicondutores (ferro fosfato). Neste caso, correções foram necessárias para o modelo da flexão termoelástica, possibilitando obter: difusividade térmica, coeficiente de difusão de portadores, velocidade de recombinação dos portadores na superfície e tempo de recombinação na superfície. As técnicas foram testadas com amostras de alumínio com 99,99 % de pureza, que possuem as informações térmicas disponíveis na literatura. Nos resultados, identificamos, através da técnica fotoacústica, que o vidro ferro fosfato é um vidro semi-condutor. Vidros ferro fosfato são candidatos para aplicações de vitrificação de resíduos nucleares. Comparações foram feitas com vidros borossilicato que são atualmente usados na vitrificação dos resíduos nucleares. Obtivemos a difusividade térmica, a capacidade térmica volumétrica e a condutividade térmica dos vidros do simulado lunar JSC-1 e telurito. O primeiro se mostrou eficiente para aplicações em exploração espacial e o segundo tem potencial aplicação em dispositivos fotônicos. / In this work we present the implantation of two photothermal techniques : the open cell photoacoustic which allows one to find thermal diffusivity of materials, and pc technique which gives the value of the product of density by specific heat of substance, known as the volumetric heat capacity. We also used the technique of thermal lens for measurement of thermal diffusivity and the parameter dS/dT (the temperature coefficient of the optical path S). The mentioned techniques furnished the thermo-optical parameters (Thermal Diffusivity, Thermal Conductivity and dS/dT) of glassy materials such as iron phosphate, tellurite, borosilicate glasses and lunar simulate JSC-1. Theoretical Models are presented and tested. It was shown that the model of thermoelastic bending is dominant in most samples studied. Exception is observed in the case of semiconducting glasses (iron phosphate). In this case, corrections were necessary to the bending model, and allowed one to obtain: thermal diffusivity, carrier 's diffusion coefficient, carriers surface recombination velocity and surface recombination time. Techniques were tested with aluminum samples with 99.99 % purity, which have the thermal information available in the literature. As a result, we identified, through the photoacoustic technique, that iron phosphate glass is a semiconductor glass. Iron phosphate are candidates for nuclear waste vitrification applications. Comparison was made with borosilicate glasses that are currently used for nuclear waste vitrification. We also obtained the thermal diffusivity, the volumetric heat capacity and thermal conductivity of simulated lunar JSC-1 and tellurite glasses. The former proved efficient applications in space exploration and the latter has potential applications as photonic device.

L’imagerie photoacoustique est une nouvelle modalité couplant imagerie optique et échographie. Non invasive, elle permet d’imager des absorbeurs optiques à quelques centimètres de profondeur et avec la résolution de l’échographie. La réception des signaux photoacoustiques se faisant à l’aide d’un échographe clinique, cette modalité hybride vient compléter idéalement l’imagerie ultrasonore en apportant des informations fonctionnelles aux informations structurelles de l’échographie. Ces atouts en font une technique d’imagerie très prometteuse pour la clinique, notamment comme outil de diagnostic précoce. Ce travail de thèse a pour objectif principal la mise en place des outils nécessaires au développement de cette thématique de recherche d’un point de vue expérimental, à des fins cliniques. En particulier, l’apport de l’imagerie photoacoustique pour le diagnostic de plaques d’athérome vulnérables est investigué sur fantômes, grâce à un protocole original. Pour cela un système d’imagerie photoacoustique a été développé et caractérisé à l’aide de fantômes bimodalités élaborés spécifiquement pour les différentes études présentées. Gardant à l’esprit le transfert de cette technique en clinique, un échographe clinique de recherche est utilisé et différentes spécificités du banc nécessaires à l’imagerie in vivo et au diagnostic médical ont été investiguées. Cela implique une amélioration des performances de détection du signal photoacoustique, notamment en termes de sensibilité et de contraste. Pour cela, une nouvelle technologie de sondes ultrasonores est évaluée en la comparant aux sondes actuellement utilisées. De plus, une excitation multispectrale permet l’identification de différents éléments présents dans les tissus. L’aspect temps-réel de l’échographie fait de cette modalité une des plus utilisées pour le diagnostic clinique. Par conséquent, une imagerie photoacoustique voire bimodale en temps réel présente un réel atout pour son transfert clinique. Cette possibilité est investiguée sur le système mis en place au cours de la thèse grâce à un échographe de recherche et une étude sur fantômes. Enfin, une autre contribution de ce travail concerne l’apport de l’imagerie photoacoustique à la caractérisation de la vulnérabilité de la plaque d’athérome. Cette indication de vulnérabilité est obtenue en déterminant la composition de la plaque, en particulier en termes de lipides. L’imagerie photoacoustique, couplée à l’échographie, peut permettre cette identification. Pour étudier cette possibilité, nous nous sommes intéressés à l’artère carotide pour son accessibilité et la place qu’elle occupe dans le diagnostic de la plaque d’athérome en échographie et échographie Doppler. Un protocole original a été élaboré afin d’apporter l’excitation optique au plus près de la carotide. La faisabilité de cette approche est investiguée sur un fantôme conçu spécifiquement pour cette étude et les résultats préliminaires sont présentés. / Photoacoustic (PA) imaging is a new imaging modality coupling ultrasound and optical imaging. This non-invasive technique achieves a penetration depth up to several centimeters with optical contrast and ultrasound resolution. Moreover, since PA signals are detected with a US scanner, PA imaging ideally complete US imaging, adding functional information to the structural ones brought by echography. Therefore PA imaging looks very promising, specifically as a clinical early diagnosis tool. The main objective of this thesis is to set up the required tools to develop the experimental investigation for this research topic and, in particular, to apply it to the diagnosis of vulnerable atheroma plaques. A PA imaging system has been set up and characterized using specifically designed bimodal phantoms. Additional studies have been made to evaluate the suitability of this imaging platform for clinical imaging. For example, in vivo imaging requires better signal detection in terms of contrast and sensitivity, achieved thanks to a new probe technology, and the identification of tissue composition using a multispectral optical excitation. Finally, PA and even PAUS real time imaging is a real asset for medical diagnosis that has been investigated. Another contribution of this work is the use of PA imaging to characterized atheroma plaques vulnerability with the detection of lipids inside these plaques. PA imaging, coupled to echography, can address this need. To study this possibility, the carotid artery has been considered and a new protocol has been elaborated to bring the optical excitation very close to this artery. A feasibility study has been realized on a specific phantom and the preliminary results are presented.

La distinction entre les fœtus constitutionnellement petits de ceux qui présentent une réelle restriction de croissance liée à une insuffisance placentaire n’est pas aisée avec les mesures échographiques utilisées en pratique courante. Le retard de croissance intra-utérin (RCIU) est responsable d’une part importante de la prématurité induite, et d’une augmentation du risque de mortalité et de morbidité néonatales. C’est pourquoi, l’amélioration de la connaissance de la vascularisation placentaire est indispensable pour mieux identifier et prendre en charge les situations d’hypoxie chroniques foetales associées à l’insuffisance placentaire.Pour quantifier la vascularisation les modalités d’imagerie de perfusion disponibles sont l’échographie et l’IRM. Les études évaluant la quantification de la perfusion placentaire par échographie de contraste sont peu nombreuses. Les avantages et les limites de cet examen ont été évalués sur un modèle murin de RCIU par ligature vasculaire. Ainsi, l’échographie de contraste permettait de quantifier une baisse de la perfusion placentaire sur un modèle de RCIU sans que l’on puisse observer de passage d’agents de contraste ultrasonores au travers la barrière placentaire. Les résultats obtenus ont été comparés aux données obtenues par l’IRM de perfusion. Les paramètres quantitatifs obtenus à partir des courbes de cinétiques du contraste pour chacune des deux modalités d’imagerie étaient comparables sur un modèle identique de RCIU murin. Enfin, une méthode d’étude de l’oxygénation placentaire par imagerie photoacoustique a été évaluée. Cette modalité d’imagerie non invasive permettait d’obtenir en temps réel l’oxygénation placentaire, avec cependant une profondeur limitée d’exploration. Le placenta semblait se comporter comme une réserve en oxygène au cours de l’étude d’une séquence hypoxie – hyperoxygénation maternelle avec une désaturation moins importante que celle observée dans les autres tissus maternels. / To identify fetuses small for their gestational-age who have reached their appropriate growth potential from growth-restricted fetuses due to placental insufficiency is uneasy. Intra Uterine Growth Restriction (IUGR) increases the risk for indicated preterm delivery, neonatal mortality and morbidity. Therefore, improving the knowledge of the placental perfusion is essential to better identify and manage fetal chronic oxygen deprivation associated with placental insufficiency.Contrast Enhanced Ultrasound (CEUS) and MRI are two imaging modalities available to quantify placental perfusion. However, few studies focus on the quantification of placental perfusion with CEUS. First, the advantages and limitations of CEUS were presented in an IUGR rat model by uterine ligation. The placental perfusion observed by CEUS was significantly decreased in the ligated horn. No contrast enhancement was observed in the umbilical vein or the fetus. Then, we compared the CEUS parameters to results obtained by MRI perfusion. Perfusion parameters were obtained from the signal intensity decay curve for the two imaging modalities. Results of such perfusion parameters were comparable in the same IUGR rat model. Finally, we evaluated the response of the placenta to oxygenation by photoacoustic imaging. PA imaging is a real-time, non-invasive method to evaluate placental oxygenation without contrast agents. Our results suggesting that placenta is less affected than maternal tissue by the decline in maternal oxygenation. The placenta may play an important role in protecting the feus against hypoxia.

The feasibility of FTIR-based spectroscopy as a tool to measure cellular response to therapeutics was investigated. Fourier transform mid-infrared spectroscopy has been used in conjunction with multivariate analysis (MVA) to assess the chemistry of many clinically relevant biological materials; however, the technique has not yet found its place in a clinical setting. One issue that has held the technique back is due to the spectral distortions caused by resonant Mie scattering (RMieS), which affects the ability to confidently assign molecular assignments to the spectral signals from biomaterials. In the light of recently improved understanding of RMieS, resulting in a novel correction algorithm, the analytical robustness of corrected FTIR spectra was validated against multi-discipline methods to characterise a set of renal cell lines which were selected for their difference in morphology.After validation of the FTIR methodology by discriminating different cell lines, the second stage of analyses tested the sensitivity of FTIR technique by determining if discrete chemical differences could be highlighted within a cell population of the same origin. The renal carcinoma cell line 2245R contains a sub-population to contain a sub-population of cells displaying 'stem-cell like' properties. These stem-like cells, however, are difficult to isolate and characterise by conventional '-omic' means. Finally, cellular response to chemotherapeutics was investigated using the established renal cell lines CAKI-2 and A-498. For the model, 5-fluorouracil (5FU), an established chemotherapeutic agent with known mechanisms of action was used. Novel gold-based therapeutic compounds were also assessed in parallel to determine their efficacy against renal cell carcinoma. The novel compounds displayed initial activity, as the FTIR evidence suggested compounds were able to enter the cells in the first instance, evoking a cellular response. The long-term performance, tracked with standard proliferation assays and FTIR spectroscopy in the renal cancer cell model, however, was poor. Rather than dismissing the compounds as in-active, the compounds may simply be more effective in cancer cell types of a different nature. The FTIR-based evidence provided the means to suggest such a conclusion. Overall, the initial results suggest that the combination of FTIR and MVA, in the presence of the novel RMieS-EMSC algorithm can detect differences in cellular response to chemotherapeutics. The results were also in-line with complimentary biological-based techniques, demonstrating the powerful potential of the technique as a promising drug screening tool.

La spectrométrie photoacoustique QEPAS constitue l’une des méthodes les plussensibles pour la détection de gaz à l’état de traces. Ses performances sont étroitement liées àcelles de sa source de lumière infrarouge cohérente et de son résonateur mécanique qui détecteles ondes acoustiques. La thèse a pour objectif de développer ces deux briques élémentaires.Dans un premier temps, les performances des résonateurs mécaniques sont modélisées, permettantde mieux comprendre leur comportement. Une formule analytique originale de leurfacteur de qualité y est incorporée, permettant de prédire avec précision les pertes qu’ils subissentlorsqu’ils résonnent dans un gaz. Grâce à ces modèles, de nouveaux résonateurs optimiséssont conçus et réalisés, aboutissant à des performances améliorées. Dans un secondtemps, les sources cohérentes infrarouges QCL et OPO sont améliorées pour la photoacoustique.L’impulsion de pompe optimale pour un OPO est présentée pour distribuer au mieuxl’énergie de pompe disponible dans le temps, et ainsi maximiser le rendement de rayonnementinfrarouge disponible. Un logiciel de simulation numérique original des OPOs est égalementcréé, et permet de simuler rapidement le spectre d’émission d’un OPO quelconque. / Infrared photoacoustic spectrometry QEPAS is one of the most sensitive techniquefor trace gas sensing. The goal of the thesis is to improve the two key elements of the instrument: the mechanical resonator and the coherent infrared light source.First, the use of resonators as an acoustic waves sensor is investigated, allowing to better understandtheir behavior. Our modeling include a new analytical formula of their quality factor,predicting the amount of losses they experience when immersed within a gaz. The models areused to design and fabricate new custom resonators, leading to enhanced performances. Second,two infrared sources named QCL and OPO are optimized for the photoacoustic application.The optimal pump pulse for an OPO is derived to efficiently distribute the available pumpenergy in time, hence maximizing the yield of infrared light. A simulation software has alsobeen created for OPOs, able to quickly predict the spectrum of any type of OPO.

The focus of the thesis is on the development of a few stochastic search schemes for inverse problems and their applications in medical imaging. After the introduction in Chapter 1 that motivates and puts in perspective the work done in later chapters, the main body of the thesis may be viewed as composed of two parts: while the first part concerns the development of stochastic search algorithms for inverse problems (Chapters 2 and 3), the second part elucidates on the applicability of search schemes to inverse problems of interest in tomographic imaging (Chapters 4 and 5). The chapter-wise contributions of the thesis are summarized below. Chapter 2 proposes a Monte Carlo stochastic filtering algorithm for the recursive estimation of diffusive processes in linear/nonlinear dynamical systems that modulate the instantaneous rates of Poisson measurements. The same scheme is applicable when the set of partial and noisy measurements are of a diffusive nature. A key aspect of our development here is the filter-update scheme, derived from an ensemble approximation of the time-discretized nonlinear Kushner Stratonovich equation, that is modified to account for Poisson-type measurements. Specifically, the additive update through a gain-like correction term, empirically approximated from the innovation integral in the filtering equation, eliminates the problem of particle collapse encountered in many conventional particle filters that adopt weight-based updates. Through a few numerical demonstrations, the versatility of the proposed filter is brought forth, first with application to filtering problems with diffusive or Poisson-type measurements and then to an automatic control problem wherein the exterminations of the associated cost functional is achieved simply by an appropriate redefinition of the innovation process. The aim of one of the numerical examples in Chapter 2 is to minimize the structural response of a duffing oscillator under external forcing. We pose this problem of active control within a filtering framework wherein the goal is to estimate the control force that minimizes an appropriately chosen performance index. We employ the proposed filtering algorithm to estimate the control force and the oscillator displacements and velocities that are minimized as a result of the application of the control force. While Fig. 1 shows the time histories of the uncontrolled and controlled displacements and velocities of the oscillator, a plot of the estimated control force against the external force applied is given in Fig. 2. (a) (b) Fig. 1. A plot of the time histories of the uncontrolled and controlled (a) displacements and (b) velocities. Fig. 2. A plot of the time histories of the external force and the estimated control force Stochastic filtering, despite its numerous applications, amounts only to a directed search and is best suited for inverse problems and optimization problems with unimodal solutions. In view of general optimization problems involving multimodal objective functions with a priori unknown optima, filtering, similar to a regularized Gauss-Newton (GN) method, may only serve as a local (or quasi-local) search. In Chapter 3, therefore, we propose a stochastic search (SS) scheme that whilst maintaining the basic structure of a filtered martingale problem, also incorporates randomization techniques such as scrambling and blending, which are meant to aid in avoiding the so-called local traps. The key contribution of this chapter is the introduction of yet another technique, termed as the state space splitting (3S) which is a paradigm based on the principle of divide-and-conquer. The 3S technique, incorporated within the optimization scheme, offers a better assimilation of measurements and is found to outperform filtering in the context of quantitative photoacoustic tomography (PAT) to recover the optical absorption field from sparsely available PAT data using a bare minimum ensemble. Other than that, the proposed scheme is numerically shown to be better than or at least as good as CMA-ES (covariance matrix adaptation evolution strategies), one of the best performing optimization schemes in minimizing a set of benchmark functions. Table 1 gives the comparative performance of the proposed scheme and CMA-ES in minimizing a set of 40-dimensional functions (F1-F20), all of which have their global minimum at 0, using an ensemble size of 20. Here, 10 5 is the tolerance limit to be attained for the objective function value and MAX is the maximum number of iterations permissible to the optimization scheme to arrive at the global minimum. Table 1. Performance of the SS scheme and Chapter 4 gathers numerical and experimental evidence to support our conjecture in the previous chapters that even a quasi-local search (afforded, for instance, by the filtered martingale problem) is generally superior to a regularized GN method in solving inverse problems. Specifically, in this chapter, we solve the inverse problems of ultrasound modulated optical tomography (UMOT) and diffraction tomography (DT). In UMOT, we perform a spatially resolved recovery of the mean-squared displacements, p r of the scattering centres in a diffusive object by measuring the modulation depth in the decaying autocorrelation of the incident coherent light. This modulation is induced by the input ultrasound focussed to a specific region referred to as the region of interest (ROI) in the object. Since the ultrasound-induced displacements are a measure of the material stiffness, in principle, UMOT can be applied for the early diagnosis of cancer in soft tissues. In DT, on the other hand, we recover the real refractive index distribution, n r of an optical fiber from experimentally acquired transmitted intensity of light traversing through it. In both cases, the filtering step encoded within the optimization scheme recovers superior reconstruction images vis-à-vis the GN method in terms of quantitative accuracies. Fig. 3 gives a comparative cross-sectional plot through the centre of the reference and reconstructed p r images in UMOT when the ROI is at the centre of the object. Here, the anomaly is presented as an increase in the displacements and is at the centre of the ROI. Fig. 4 shows the comparative cross-sectional plot of the reference and reconstructed refractive index distributions, n r of the optical fiber in DT. Fig. 3. Cross-sectional plot through the center of the reference and reconstructed p r images. Fig. 4. Cross-sectional plot through the center of the reference and reconstructed n r distributions. In Chapter 5, the SS scheme is applied to our main application, viz. photoacoustic tomography (PAT) for the recovery of the absorbed energy map, the optical absorption coefficient and the chromophore concentrations in soft tissues. Nevertheless, the main contribution of this chapter is to provide a single-step method for the recovery of the optical absorption field from both simulated and experimental time-domain PAT data. A single-step direct recovery is shown to yield better reconstruction than the generally adopted two-step method for quantitative PAT. Such a quantitative reconstruction maybe converted to a functional image through a linear map. Alternatively, one could also perform a one-step recovery of the chromophore concentrations from the boundary pressure, as shown using simulated data in this chapter. Being a Monte Carlo scheme, the SS scheme is highly parallelizable and the availability of such a machine-ready inversion scheme should finally enable PAT to emerge as a clinical tool in medical diagnostics. Given below in Fig. 5 is a comparison of the optical absorption map of the Shepp-Logan phantom with the reconstruction obtained as a result of a direct (1-step) recovery. Fig. 5. The (a) exact and (b) reconstructed optical absorption maps of the Shepp-Logan phantom. The x- and y-axes are in m and the colormap is in mm-1. Chapter 6 concludes the work with a brief summary of the results obtained and suggestions for future exploration of some of the schemes and applications described in this thesis.

Filmes de poli(fluoreto de vinilideno-co-trifluoretileno), P(VDF-IrFE), com uma razão molar 70/30 de VDF e IrFE, respectivamente, foram expostos à radiação-X sob vácuo em uma ampla faixa de doses de irradiação. Este é um copolímero estatístico e semi-cristalino que possui a especial característica de cristalizar espontaneamente numa estrutura ferroelétrica. Ele também possui uma transição de fase ferro-paraelétrica detectável, definida como a temperatura de Curie (Tc). Devido a estas características tem despertado considerável interesse, em especial na área da eletrônica como elemento transdutor. As modificações induzidas foram investigadas por espectroscopia fotoacústica no infravermelho (FT-IR/PAS), assim como FI-IR por transmitância, calorimetria exploratória diferencial (DSC), termogravimetria (IG), difração de raios-X, UV/Visível e espectroscopia Raman. As técnicas espectroscópicas vibracionais (fotoacústica no IR, Raman e absorção no IR) foram utilizadas na identificação de bandas relacionadas às regiões cristalinas e amorfas, formação e rompimento de ligações e presença de novos grupos funcionais. Nos espectros IR e Raman são observadas duas bandas que estão relacionadas às regiões cristalinas e sofrem mudanças nas suas intensidades relativas de acordo com a dose de radiação. Essas mudanças podem ser interpretadas como aumento ou diminuição do grau de cristalinidade, e também em termos de modificações de arranjos cristalinos. A difração de raio-X mostrou o aparecimento de um pico, próximo àquele da fase ferroelétrica, sob aumento da dose de radiação, devido a um processo de modificação do arranjo cristalino acima da dose de 480 kGy. Foi observado um aumento de intensidade no referido pico de difração, correspondendo a um aumento do grau de cristalinidade da amostra. As curvas de DSC mostraram picos endotérmicos correspondentes a fusão e transições de fases que, através de suas variações, possibilitam avaliar os efeitos da irradiação com raios-X. Os espectros UV/Visível mostraram absorções dos cromóforos cujas intensidades de banda aumentam com a dose de radiação e diminuem durante o envelhecimento da amostra. Os dados indicam que a radiação-X induz uma modificação no arranjo cristalino do P(VDF-TrFE). Tal modificação, é provavelmente uma mudança de estrutura ferroelétrica para outra, paraelétrica. / Poly(vinylidene fluoride-co-trifluoroethylene) films, P(VDF-TrFE), with a molar ratio 70/30 of VDF and TrFE units, respectively, were exposed to X-ray radiation under vacuum in a wide range of irradiation doses. This is a statistic semi-crystalline copolymer and displays the unique feature of a spontaneous crystallization into a ferroelectric structure. It also possesses a detectable ferro-paraelectric transition, the Curie temperature (Tc). Due to these characteristics considerable interest in such copolymer has been generated, specially in electronics as a transducer element. The induced modifications were investigated by Fourier transform infrared photoacoustic spectroscopy (FT-IR/PAS) as well as transmittance FT-IR, differential scanning calorimetry (DSC), thermogravimetry (TG), X-ray diffraction, UV/Visible and Raman spectroscopies. The spectroscopic vibrational techniques (FT-IR/PAS, FT-IR and Raman) were used to identify bands related to crystalline and amorphous regions, bond formation, bond scission and presence of new functional groups. In both IR and Raman spectra were observed a couple of bands related to the crystalline regions that undergo changes of relative intensities with the radiation dose. These changes may be interpreted as an increase or decrease of the crystallinity degree, and also modifications of crystal structure. X-ray diffraction showed a new peak, close to that of the ferroelectric phase, under increasing radiation doses, due to a modification of crystal structure process above 480 kGy dose. An increase in the intensity of the former diffraction peak was observed, corresponding to an increase in the crystallinity degree. The DSC curves showed the endothermic peaks corresponding to the melting and the phase transitions, whose variations allow an evaluation of the effects of X-ray radiation. UV/Visible spectra showed chromophores absorptions whose band intensities increase by radiation dose and decrease during sample\'s aging. The data indicate that P(VDF-TrFE) under X-ray radiation exposition undergoes a crystal structure modification, probably a change of a ferroelectric structure to another one, paraelectric.

À cause de leur diffusion et de leur absorption des radiations solaires, les aérosols atmosphériques jouent un rôle important dans l'évolution du climat terrestre. Les techniques de mesure actuelles apportent certes, des connaissances, sur le forçage radiatif mais les résultats possèdent généralement de larges incertitudes, souvent du même ordre de grandeur que la valeur elle-même. Ces incertitudes sont causées par le manque de précision sur les données liées aux propriétés optiques estimées de ces aérosols (comme l'absorption, la diffusion ou l'extinction). Elles découlent principalement des techniques de mesures actuelles : à l'effet de chargement des filtres (lors de mesures classiques par filtres), aux mesures limitées par l'étendue spectrale des instruments, aux conditions d'échantillonnage différents lors de mesures séparées, etc. Dans ce travail de thèse, j'ai développé puis testé des instruments optiques et électroniques dans le but d'augmenter la précision des mesures des coefficients d'extinction et d'absorption des aérosols. (1) Deux spectrophones PhotAccoustique (PA) sont développés afin d'améliorer les mesures d'absorption des aérosols grâce à des mesures directes et sans filtres. Une première génération utilisant un rayonnement à 444 nm permet de réduire les incertitudes de mesure de 20-30% (obtenue par la technique d'échantillonnage par filtres) à 7,4% et 4,6% pour la détermination des coefficients d'absorption massique du carbone suie et de cendres volcaniques, respectivement. Transformé en spectrophone PA à multi-longueurs d'onde opérant conjointement à 444,532 et 660 nm, il permet alors de caractériser la dépendance spectrale du Coefficient d'Absorption d'Ångström (CAA). Les valeurs du CAA du carbone suie sont en accord avec les résultats publiés. Celles obtenues lors de l'analyse de deux échantillons de cendres volcaniques résultant de l'éruption du Eyjafjallajökull sont similaires au CAA du carbone brun,prouvent la présence d'importantes quantités d'éléments organiques. (2) Un extinctiomètre, basé sur le principe de la spectroscopie d'absorption en cavité à source large bande et incohérente (IBBCEAS), est ensuite développé afin de suivre l'évolution des propriétés optiques d'Aérosols Organiques Secondaires (AOS) produits par la photolyse du 2-nitrophénol dans une chambre de simulation atmosphérique de l'University College de Cork (Irlande). Leurs coefficients d'extinction et d'absorption sont suivis par cet extinctiomètre et un spectrophone PA durant tout le processus de production. Les évolutions des propriétés optiques des AOS confirment l'effet du vieillissement atmosphérique. (3) Une nouvelle architecture de détection synchrone est développé afin de rendre notre prototype plus léger, plus compact, mieux adapté aux applications in situ et plus particulièrement aux drones, techniques émergentes qui permettent de caractériser le profil vertical des aérosols dans l'atmosphère. Cette détection synchrone innovante, évaluée lors de la mesure de la concentration de NO₂ ambiant (niveau de concentration de quelques ppbv) possède une précision et une reproductibilité de mesures comparable à la détection synchrone SR830, commercialisée par la société Stanford Research Inc. L'évaluation précise de l'impact climatique des aérosols nécessite une quantification exacte et non biaisée de leurs propriétés optiques. À ce jour, elle reste un défi majeur dans la recherche sur les sciences de l'atmosphère et du changement climatique. Ainsi, des informations sur la taille des particules (liée à l'absorption sélective en longueur d'onde) nécessitent des mesures étendues sur de larges régions spectrales du rayonnement solaire principale. Le développement d'un albédomète large bande à haute précision, dédié à la mesure simultanée des coefficients d'extinction et d'absorption des aérosols est en cours. / Atmospheric aerosols are known to play an important role in earth climate by scattering and absorbing solar radiation. However, the aerosol radiative forcing effect is still known with large uncertainties (almost equal to the magnitude of the aerosol radiative forcing). The uncertainties are mainly caused by inaccurate estimates of aerosol optical properties (such as its absorption, scattering and extinction coefficients) using the currently available measurement techniques, with result in filter loading effect in classic filter technique, the uncertainty due to different sampling conditions for separate measurements of aerosol optical properties in combination of different techniques or due to the measurements at limited spectral wavelength ranges. My PhD work was carried out on the developments and applications of optical and electronic instruments for accurate measurements of aerosol extinction and absorption coefficient : (1) Photoacoustic spectrophones were developed for filter-free direct measurements of aerosol absorption with high accuracy. Measurements uncertainties down to about 7.4% and 4.6% (compared to about 20-30% in filter-based measurements) were achieved for the determination of mass absorption coefficients of black carbon and volcanic ash samples, respectively, using a single-wavelength PA spectrophone operating at 444 nm. A 3-wavelength PA spectrophone operating at 444,532 and 660 nm was developed and deployed for characterizing wavelength-dependent optical properties of aerosol absorption Ångström coefficient (AAC). The determined AAC of black carbon was well consistent with the previously reported value. Our AAC values of two volcanic ash samples from 2010 eruptions of Eyjafjallajökull, similar to the AAC of brown carbon, indicated abundant organic compounds in the volcanic ash samples. The developed multi-wavelength PA spectrophone was tested and validated in an intensive field campaign measurements of environmental particles in Grenoble (France). Side-by-side inter-comparison measurements using an aethalometer showed a lineat correlation of the measured aerosol absorption coefficients from both instruments. (2) An extinctiometer based on IBBCEAS was developed for study of optical properties of secondary organic aerosol (SOA) produced from photolysis of 2-nitrophenol in an atmospheric simulation chamber at University College Cork (Ireland). Simultaneous monitoring of the SOA extinction and absorption (in conjuction with a PA spectrophone) coefficients was performed during its whole production process, the measured evolutions of the SOA optical properties highlighted the atmospheric aging effect. (3) In order to render optical sensor lightweight and suitable for field applications, in particular for the newly emerging unmanned aerial vehicle (UAV) applications, a novel architecture of lock-in amplifier (LIA) was proposed and developed in the framework of this Phd Research. The novel LIA, evaluated with an inter-comparison measurement of ambient NO₂ at the ppbv concentration level, shows an identical performance (in terms of measurements accuracy and precision) as the widely used commercial LIA (SR830, Stanford Research Inc.), while using a simplified and lightweight hardware architecture. Evaluation of the aerosol impact on climate requires accurate and unbiased quantification of the its wavelength-dependent optical properties over a wide spectral region of the major solar radiation, which can provide information on particle size (due to the wavelength dependence of scattering by fine particles) as well as insights on aerosol chemical composition (because of its wavelength selective absorption). To date, it is still a key challenge in atmospheric science and climate change research. Development of a broadband aerosol albedometer is ongoing, which is dedicated to simultaneous measurements of aerosol extinction and absorption coefficients with high-accuracy and high-precision.