In this Thesis, two problems were studied: a direct vacuum acceleration of electrons by a tightly focused ultrashort relativistic laser pulse and ion acceleration in the process of spherical laser-heated plasma explosion. The electromagnetic field of a tightly focused laser pulse was evaluated numerically by means of Stratton-Chu integrals. The properties of the focused field were analyzed in detail for a plane wave or a macroscopically large Gaussian beam incident onto the mirror. Free electrons moving in the tightly focused field were found to accelerate by two possible mechanisms: focal spot acceleration and capture-and-acceleration scenario. The two mechanisms were studied in detail. Comparison of the mirror-focused field with first- and fifth-order paraxial fields is performed. A 3D electromagnetic PIC code SCPIC was created for simulations of pulse interaction with targets having a finite number of particles interacting with each other by collective fields. Atto-second bunch formation was observed in the interaction with ultra-small or ultra-thin targets. Physical mechanism of bunch formation is explained. The problem of electrostatic explosion of a nano-scale spherical plasma with initially hot electrons and cold ions was solved numerically. Expansion in a wide regime of electron temperature $0 < T leq infty$ was studied in detail for different initial density profiles of plasma. Favorable conditions for obtaining mono-energetic ions resulting from the explosion were specified in single and two ionic species cases. In case of a two-species explosion, the number of mono-energetic, $deltavarepsilon/varepsilon < 10\%$, ions can be as high as 70-80\% of the total light ions for a wide range of electron temperatures.

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Neste trabalho, apresentamos um estudo detalhado da técnica de desaceleração e aceleração de átomos pelo ajuste Zeeman, possibilitando a produção de um feixe atômico monoenergético. Usando esta técnica, realizamos estudos sobre efeito de bombeameto óptico e condições de seguimento adiabático dos átomos no campo magnético. Através do entendimento destes efeitos, pudemos propor modificações que permitirão a produção de um fluxo intenso de átomos monoenergéticos, que deverão permitir experimentos, com este tipo de feixe atômico, fora do sistema / We have carefully studied the Zeeman-tuned technique to decelerate and also accelerate sodium atoms atomic beam, creating ways of producing monoenergetic atomic beams. A systematic study of the optical pumping effects on these beams, as well as its adiabatic following conditions along the magnetic field were also investigated. A single laser beam, together with minor changes on the the magnetic field profile and on the optical setup, was used to decelerate and/or to accelerate atoms running outside of the Zeeman solenoid, simplifying and speeding up the experimental runs

Neste trabalho, apresentamos um estudo detalhado da técnica de desaceleração e aceleração de átomos pelo ajuste Zeeman, possibilitando a produção de um feixe atômico monoenergético. Usando esta técnica, realizamos estudos sobre efeito de bombeameto óptico e condições de seguimento adiabático dos átomos no campo magnético. Através do entendimento destes efeitos, pudemos propor modificações que permitirão a produção de um fluxo intenso de átomos monoenergéticos, que deverão permitir experimentos, com este tipo de feixe atômico, fora do sistema / We have carefully studied the Zeeman-tuned technique to decelerate and also accelerate sodium atoms atomic beam, creating ways of producing monoenergetic atomic beams. A systematic study of the optical pumping effects on these beams, as well as its adiabatic following conditions along the magnetic field were also investigated. A single laser beam, together with minor changes on the the magnetic field profile and on the optical setup, was used to decelerate and/or to accelerate atoms running outside of the Zeeman solenoid, simplifying and speeding up the experimental runs

<p>Light-ions (protons, deuterons, tritons, ³He and α articles) production in the interaction of 175 MeV neutrons with iron and bismuth has been measured using the Medley setup at the The Svedberg Laboratory (TSL) in Uppsala. These measurements have been conducted in the frame of an international collaboration whose aim is to provide the scientific community with new nuclear data of interest for the development of Accelerator Driven Systems, in the range of 20 to 200 MeV. In this Licentiate Thesis I will present the background for the present experiment, the choice of the measured materials (iron and bismuth) and of the energy range. I will then give a short theoretical description of the involved nuclear reactions and of the model used to compare the experimental results. A description of the neutron facility at TSL and of Medley setup will follow. Monte Carlo simulations of the experimental setup have been performed and some results are here reported and discussed. I will present data reduction procedure and finally I will report preliminary double differential cross sections for production of hydrogen isotopes from iron and bismuth at several emission angles. Experimental data will be compared with model calculations with TALYS-1.0; these show better agreement for the production of protons, while seems to overestimate the experimental production of deuterons and tritons.</p>

Light-ions (protons, deuterons, tritons, 3He and α articles) production in the interaction of 175 MeV neutrons with iron and bismuth has been measured using the Medley setup at the The Svedberg Laboratory (TSL) in Uppsala. These measurements have been conducted in the frame of an international collaboration whose aim is to provide the scientific community with new nuclear data of interest for the development of Accelerator Driven Systems, in the range of 20 to 200 MeV. In this Licentiate Thesis I will present the background for the present experiment, the choice of the measured materials (iron and bismuth) and of the energy range. I will then give a short theoretical description of the involved nuclear reactions and of the model used to compare the experimental results. A description of the neutron facility at TSL and of Medley setup will follow. Monte Carlo simulations of the experimental setup have been performed and some results are here reported and discussed. I will present data reduction procedure and finally I will report preliminary double differential cross sections for production of hydrogen isotopes from iron and bismuth at several emission angles. Experimental data will be compared with model calculations with TALYS-1.0; these show better agreement for the production of protons, while seems to overestimate the experimental production of deuterons and tritons.

A Tomografia Computadorizada de Energia Dupla (DECT em inglês) é um dos campos das imagens tomográficas que mais evoluiu nos últimos anos. O DECT usa dois espectros para irradiar pacientes e é capaz de diferenciar tecidos com base na sua composição elementar. Apesar de serem semelhantes aos dispositivos padrão de tomografia, para essa modalidade é necessário o desenvolvimento de ferramentas específicas que permitam o estudo de suas propriedades de imagem. O objetivo deste trabalho era construir um sistema simulado de Tomografia Computadorizada (TC) com a capacidade de produzir imagens semelhantes às obtidas em dispositivos DECT reais. O TC simulado também permitiria explorar as propriedades das imagens de materiais de teste antes de sua construção física. Este trabalho presenta a simulação do processo de aquisição de imagens de um dispositivo DECT que funciona a partir da troca rápida de kV, o GE Discovery CT 750 HD. A geometria simulada foi baseada num dispositivo atualmente disponível no InRad (Instituto de Radiologia da Faculdade de Medicina da Universidade de São Paulo). As simulações foram realizadas usando o código Monte Carlo PENELOPE/penEasy para simular o transporte de radiação através dos materiais e detectores. Também é apresentada uma comparação entre as imagens obtidas no dispositivo real e nas simulações. Para isso, foi preparado um objeto simulador cilíndrico contendo concentrações de materiais equivalentes a iodo e cálcio. As imagens de tal objeto simulador foram adquiridas no equipamento GE Discovery CT 750 HD. Um objeto simulador equivalente foi modelado e as suas imagens foram simuladas com o código PENELOPE/penEasy. As imagens foram adquiridas e reconstruídas de acordo com as possibilidades do equipamento clínico de tomografia. Imagens de concentração de material e imagens monoenergéticas foram obtidas a partir do dispositivo CT clínico e das simulações. O algoritmo BMD (Basis Material Decomposition em Inglês) baseado nas projeções foi implementado usando os coeficientes de atenuação mássicos da água e do iodo. Consequentemente, imagens de concentração dos materiais água e iodo foram obtidas. A concentração medida nos cilindros de iodo foi equivalente às esperadas tanto no dispositivo real quanto nas imagens simuladas. Foram observados artefatos de endurecimento de feixe nas imagens de concentração de material. Imagens monoenergéticas foram obtidas para diferentes energias. Tais imagens foram obtidas a partir da superposição das imagens de concentração de água e iodo, que foram ponderadas pelos seus respectivos coeficientes de atenuação mássicos. Verificou-se que para as imagens monoenergéticas simuladas e reais em altas energias a imagem de concentração da água é a componente dominante, produzindo imagens que apresentaram as cavidades de iodo como menos atenuantes do que a água. Por outro lado, para energias baixas, a componente dominante nas imagens monoenergéticas foi a imagem de concentração do iodo. O CNR foi analisado nas imagens monoenergéticas como função da energia. As curvas do CNR dos dispositivos simulado e real exibiram semelhanças em sua forma, mas com escala diferente devido à diferença no ruído. Foi possível concluir que o modelo DECT simulado apresenta resultados qualitativos semelhantes aos obtidos no dispositivo real. O sistema de TC simulado permite explorar as características das imagens com diferentes materiais e composições. Ele também pode ser usado como uma ferramenta didática para melhorar a compreensão da diferenciação de materiais em tomografia espectral e DECT. / Dual Energy (DE) Computed Tomography (CT) is one of the fields of tomographic images that has evolved rapidly during the last years. DECT uses two X-ray spectra to irradiate patients It is capable to differentiate materials based on its elementary composition. Despite being similar to standard CT devices, DECT devices require the development of specific tools that allow the study of their image properties. The objective of this work was to build a modelled CT system capable of producing images similar to those obtained in real DECT devices. The modelled CT would also allow exploring the image properties of test materials before their physical construction. This work presents the simulation of the acquisition process of a DECT device that works with rapid kV switching, the GE Discovery CT 750 HD. The simulated geometry was based on a device currently available at the InRad (Institute of Radiology of the Faculty of Medicine of the University of São Paulo). The simulations were carried out using the PENELOPE/penEasy Monte Carlo code, which simulates radiation transport through the materials and detectors. A comparison between the images obtained in the real device and from simulations is also presented. To do so, a real phantom was prepared to be imaged and an equivalent system was simulated. The phantom contained inserts with concentrations of iodine and calcium. The images were acquired and reconstructed according to the possibilities of the real CT device. Standard, material concentration and virtual monoenergetic images were acquired[L1] from both, the real CT device and simulations. The Projection-Based BMD method was implemented using the mass attenuation coefficients of water and iodine. Then, material concentration images of water and iodine were obtained. The iodine concentrations estimated from the images agreed with the expected values in both real device and simulated images. Beam hardening artefacts were observed in the simulated material concentration images. Monoenergetic images were obtained for different energies. Such images were obtained as a superposition of the concentration images of water and iodine, weighed by their respective mass attenuation coefficient. It was verified that in the simulated and real device images, at high energies, the water concentration image predominated in the monoenergetic images, producing images that presented the iodine cavities as less attenuating than water. In contrast, at low energies, the predominant component of the monoenergetic images was the iodine concentration image. Contrast Noise Ratio (CNR) was analysed in the monochromatic images as a function of energy. Simulated and real device CNR curves exhibited similarities in their shape but with a different scale due to their difference in noise. It was possible to conclude that the simulated DECT model presented qualitative results similar to the obtained in the real device. The modelled CT system permits exploring the image features with different materials and compositions. It could also be used as a didactic tool to improve the understanding of material differentiation in spectral or DECT.

La réponse d’un détecteur de neutrons varie avec l’énergie du neutron incident. La détermination expérimentale de cette variation se réalise au moyen de champs neutroniques monoénergétiques. Ceux-ci sont produits par l’interaction entre un faisceau d’ions accélérés et une cible fine constituée d’un dépôt réactif sur un support métallique. En utilisant différentes réactions telles que 7Li(p,n), 3H(p,n), 2H(d,n) et 3H(d,n), il est possible de produire des neutrons entre 120 keV et 20 MeV dans la direction du faisceau incident (0°).Pour atteindre des énergies inférieures, il est possible d’augmenter l’angle du point de mesure par rapport à la direction du faisceau d’ions. Cependant, cette méthode présente des problèmes d’homogénéité en énergie et en fluence des neutrons à la surface du détecteur, ainsi qu’une augmentation de la proportion de neutrons diffusés. Une alternative est l’utilisation d’autres réactions nucléaires, notamment la réaction 45Sc(p,n) qui permet de descendre jusqu’à des énergies de 8 keV à 0°.Une étude complète de cette réaction et de sa section efficace a été menée au sein d’une coopération scientifique entre le laboratoire de métrologie et de dosimétrie des neutrons (LMDN) de l’IRSN, deux instituts de métrologie européens, le NPL (National Physical Laboratory, RU) et le PTB (Physikalisch-Technische Bundesanstalt, All), et l’IRMM (Institute for Reference Materials and Measurements, CEE). Parallèlement, d’autres réactions envisageables ont été étudiées : 65Cu(p,n), 51V(p,n), 57Fe(p,n), 49Ti(p,n), 53Cr(p,n) et 37Cl(p,n). Elles ont été comparées en termes d’émission neutronique et d’énergie minimale des neutrons produits. / The response of a neutron detector, defined as the reading of the device per unit of incident fluence or dose, varies with neutron energy. The experimental determination of this variation, i.e. of the response function of this instrument, has to be performed by facilities producing monoenergetic neutron fields. These neutrons are commonly produced by interaction between accelerated ions (proton or deuteron) onto a thin target composed of a reactive layer deposited on a metallic backing. Using the 7Li(p,n), 3H(p,n), 2H(d,n) and 3H(d,n) reactions, monoenergetic neutrons are obtained between 120 keV and 20 MeV in the ion beam direction (0°).To reach lower neutron energies, the angle of the measuring point with respect to the ion beam direction can be increased. However, this method presents several problems of neutron energy and fluence homogeneities over the detector surface, as well as an important increase of the scattered neutron contribution. Another solution is to investigate other nuclear reactions, as 45Sc(p,n) allowing to extend the neutron energy range down to 8 keV at 0°.A complete study of this reaction and its cross section has been undertaken within the framework of a scientific cooperation between the laboratory of neutron metrology and dosimetry (IRSN, France), two European national metrological institutes, the National Physical Laboratory (UK) and the Physikalisch-Technische Bundesanstalt (Germany), and IRMM, the Institute for Reference Materials and Measurements (EC).In parallel, other possible reactions have been investigated: 65Cu(p,n), 51V(p,n), 57Fe(p,n), 49Ti(p,n), 53Cr(p,n) and 37Cl(p,n). They were compared in terms of neutron fluence and minimum energy of the produced neutrons.

Fundação Carlos Chagas Filho de Amparo a Pesquisa do Estado do Rio de Janeiro / Um método numérico espectronodal (END) livre de erros de truncamento espacial é desenvolvido para problemas unidimensionais de difusão de nêutrons monoenergéticos em duas versões. Na versão de problemas de autovalor, o método gera soluções numéricas para o perfil do fluxo escalar e para o fator de multiplicação efetivo (k), que coincidem com a solução analítica dominante, afora os erros da aritmética finita computacional. Na versão de fonte fxa, o método também gera soluções numéricas analíticas para o problema de fonte fixa correspondente, onde a fonte de fissão, com dependência espacial, é obtida analiticamente, a partir da reconstrução espacial do fluxo escalar gerado pelo método END para problemas de autovalor. Alguns experimentos numéricos são apresentados para dois problemas modelos a fim de ilustrar a precisão do método.

Fundação Carlos Chagas Filho de Amparo a Pesquisa do Estado do Rio de Janeiro / Um método numérico espectronodal (END) livre de erros de truncamento espacial é desenvolvido para problemas unidimensionais de difusão de nêutrons monoenergéticos em duas versões. Na versão de problemas de autovalor, o método gera soluções numéricas para o perfil do fluxo escalar e para o fator de multiplicação efetivo (k), que coincidem com a solução analítica dominante, afora os erros da aritmética finita computacional. Na versão de fonte fxa, o método também gera soluções numéricas analíticas para o problema de fonte fixa correspondente, onde a fonte de fissão, com dependência espacial, é obtida analiticamente, a partir da reconstrução espacial do fluxo escalar gerado pelo método END para problemas de autovalor. Alguns experimentos numéricos são apresentados para dois problemas modelos a fim de ilustrar a precisão do método.