Polarized helium-3 is used as a contrast agent for lungs magnetic resonance imaging that has recently reached the pre-clinical applications. One method to hyperpolarize 3He is the metastability exchange optical pumping (MEOP). Optical pumping is performed in standard conditions at low pressure (~ 1 mbar) and low magnetic field (~ 1 Gauss). In this work, the complete update of a low field polarizer dedicated to small animal lungs imaging is presented. The implementation of a new 10 W laser, new peristaltic compressor and others components resulted in a production of 3-4 scc/min for a polarization between 30 to 40%. Images of rat lungs made with better resolution and a new dynamic radial sequence are presented as a validation of the system. Since few years, MEOP has also been studied at higher pressures and higher magnetic fields in small sealed cells. It showed that, thanks to hyperfine decoupling effect induced by high magnetic field, it was also possible to efficiently polarize at higher pressure (67 mbar). Experiments done at 4.7 and 1.5 T are reported in this work. The first ones show a benefic (higher polarization values) and a negative effect (lower production rates) of the magnetic field. The seconds highlight the advantage of using an annular beam shape of the laser that matches the distribution of 23S state atoms at higher pressure. Nuclear polarization values of 66.4% at 32 mbar and 31% at 267 mbar were obtained in 20 mL sealed cells and a 10 times increase in the production rate compare to best standard conditions. These promising results were the first motivation for building a high-field polarizer working inside MRI scanner in hospital. The design and the construction of such a polarizer are described in detail in the last part of the dissertation. The polarizer produces hyperpolarize 3He at 30-40% with a 4 times higher flow than the low field polarizer (10-15 scc/min). The first good quality human lungs images made in Poland with healthy volunteers are the main result of this work.

Cette thèse traite de la manipulation des deux degrés de libertés internes des molécules, que sont la rotation et la vibration. Il s'agit de transférer par un mécanisme de pompage optique les molécules formées dans plusieurs niveaux vibrationnels et rotationnels vers le niveau rovibrationnel absolu (J = v = 0). La démonstration expérimentale est effectuée sur des molécules froides de césium formées par photoassociation d'atomes froids. Le pompage optique est de plus démontré vers d'autres niveaux rotationnels du niveau vibrationnel fondamental. Le niveau cible est rendu noir par façonnage du spectre laser, c'est-à-dire que les molécules qui l'occupent ne peuvent plus absorber de photons du fait que le laser ne fournit pas les fréquences résonnantes nécessaires. Dans le cas du césium, la faible séparation en énergie entre les niveaux rotationnels nécessite une source spectralement fine. En effet, un laser large bande est dédié au refroidissement de la vibration et un second laser, plus fin spectralement, est utilisé pour le refroidissement de la rotation. La méthode démontrée est très générale. Des simulations, en très bon accord avec l'expérience, montrent qu'elle peut être appliquée à d'autres molécules. Une application à des jets moléculaires est aussi discutée. Elle pourrait permettre d'ouvrir la voie à un refroidissement laser et une collimation de jet avec d'éventuelles applications de lithographie. / The focus of this thesis is the manipulation of the internal degrees of freedom of translationally cold cesium molecules produced by photoassociation of cold atoms. Molecules formed in several vibrational and rotational levels are transferred by an optical pumping mechanism in the absolute rovibronic ground level (v = J = 0) or, alternatively, into other selected rotational levels of the electronic ground state. The main idea of the process is to make the target level not accessible ("dark") to the optical excitation. The suppression of the optical frequencies necessary to make a chosen state dark is obtained by spectral shaping of the excitation laser used for the optical pumping. Molecules present in this state cannot absorb photons because the laser does not provide the necessary resonant frequencies. While a broadband laser is dedicated to cool the vibrational degrees of freedom, a second narrowband laser is used to cool the rotational one because the small rotational splitting of Cs2 levels requires a narrowband source. This method is very general indeed. Simulations, for the cesium case are in very good agreement with the experiment, show that it can be applied to many other molecules. Furthermore, it could pave the way to the optical manipulation of molecular beams, to direct laser cooling of molecules and beam collimation with possible lithography applications.

Nous avons étudié les propriétés dynamique d'un spin individuel dans une boite quantique de semiconducteur II-VI (spin d'un atome de Mn ou electron résident). Une boîte quantique comportant un atome de manganese présente six raies qui permettent de sonder optiquement l'état de spin du Manganese. Des expériences pompe-sonde réalisées sur boîte unique ont permit de montrer que le spin du Mn peut être orienté optiquement en quelques dizaines de ns, que le temps de vie $T_1$ de ce spin est supérieur à la $mu$s, et que le pompage optique en champ nul est controlé par une anisotropie magnétique induite par les contraintes. Par ailleurs, dans le but d'identifier les mechanismes du pompage optique, nous avons mis en évidence des processus de relaxation de spin au sein du système exciton-manganese, durant la durée de vie de ce dernier. Enfin, nous avons mis en evidence un effet Stark optique sur chacune des raies d'une boîte quantique magnétique. Concernant la dynamique d'un électron dans une boîte quantique II-VI, nous avons mis en évidence le pompage du spin de l'électron résident ainsi que des noyaux. / We have studied the dynamic properties of a single spin (Mn impurity or resident electron) in a II-VI semiconductor quantum dot. A quantum dot doped with a single Mn atom presents six lines which allow to probe optically the spin-state of the Mn atom. Pump-probe experiments at a single dot level were carried out to demonstrate that the Mn spin could be oriented in a few tens of ns, and that the spin-distribution prepared by such means was perfectly conserved over a few $mu$s. The optical pumping of the Mn spin at zero magnetic field is controlled by a strain-induced magnetic anisotropy. Furthermore, seeking for a microscopic mechanism controlling the optical pumping of the Mn atom, we have evidenced spin relaxation channels within the exciton-Mn complex. At last, we have evidenced an optical Stark effect on any of the lines of a Mn-doped quantum dot. Concerning the dynamics of an electron in a II-VI quantum dot, we have evidenced optical pumping of the resident electron, and dynamic nuclear spin polarization.

<p>Since the inception of hyperpolarized 129Xe MRI, the field has yearned for more efficient production of more highly polarized 129Xe. For nearly all polarizers built to date, both peak 129Xe polarization and production rate fall far below theoretical predictions. This thesis sought to develop a fundamental understanding of why the observed performance of large-scale 129Xe hyperpolarization lagged so badly behind theoretical predictions.</p><p> This is done by thoroughly characterizing a high-volume, continuous-flow polarizer using optical cells having three different internal volumes, and employing two different laser sources. For each of these 6 combinations, 129Xe polarization was carefully measured as a function of production rate across a range of laser absorption levels. The resultant peak polarizations were consistently a factor of 2-3 lower than predicted across a range of absorption levels, and scaling of production rates deviated badly from predictions based on spin exchange efficiency.</p><p> To bridge this gap, we propose that paramagnetic, activated Rb clusters form during spin exchange optical pumping (SEOP), and depolarize Rb and 129Xe, while unproductively scattering optical pumping light. When a model was built that incorporated the effects of clusters, its predictions matched observations for both polarization and production rate for all 6 systems studied. This permits us to place a limit on cluster number density of <2 × 109 cm-3.</p><p> The work culminates with deploying this framework to identify methods to improve polarization to above 50%, leaving the SEOP cell. Combined with additional methods of preserving polarization, the polarization of a 300-mL batch of 129Xe increased from an average of 9%, before this work began, to a recent value of 34%.</p><p> We anticipate that these developments will lay the groundwork for continued advancement and scaling up of SEOP-based hyperpolarization methods that may one day permit real-time, on-demand 129Xe MRI to become a reality.</p> / Dissertation

Abstract This thesis reports simulations of direct observables in electron and nuclear spin relaxation experiments in an example paramagnetic system, as well as polarization transfer occurring in a spin-exchange optical pumping (SEOP) experiment. Studies of paramagnetic relaxation are important, e.g., in the development of agents used for enhanced contrast in magnetic resonance imaging. SEOP is used to produce hyperpolarized noble gases, which are then used to, e.g., enhance sensitivity in structural studies of matter with nuclear magnetic resonance. Presently the theory, available software and hardware for such computational modeling have reached a state in which quantitative reproduction of the experimentally observed magnetization decay is possible from first principles. The present multiscale computations are carried out from first principles combining molecular dynamics simulations of atomistic motion and quantum-chemical electronic structure calculations of the spin interaction parameters that enter the effective spin Hamiltonian. A time series of the spin Hamiltonian is then explicitly used to propagate spin dynamics in the system, and dynamical time constants of the magnetization are obtained through ensemble averaging. The complete decay of electron spin magnetization could be followed directly within the duration of the simulation, whereas the nuclear spin relaxation rates were extracted using Kubo’s theory regarding generalized cumulant expansion and stochastic processes. The extracted electron and nuclear spin relaxation rates for the chosen prototypic system, the aqueous solution of Ni²⁺, are in quantitative and semi-quantitative agreement, respectively, with the available experimental results. The simulations of polarization transfer corroborate the empirical observations on the importance of van der Waals complexes and binary collisions in the spin-exchange process. Long van der Waals complexes represent the overwhelmingly most significant kind of individual events, but the short binary collisions can also give a relatively important contribution due to their vast abundance. This thesis represents a first study in which first principles-calculated trajectories of individual events could be followed. The simulations reported in this thesis were run without any empirical parametrization and thus represent a significant step in first-principles computational modeling of magnetization dynamics.

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Submitted by Marco Antonio Oliveira da Silva (maosilva@ipen.br) on 2017-11-09T11:51:03Z No. of bitstreams: 0 / Made available in DSpace on 2017-11-09T11:51:03Z (GMT). No. of bitstreams: 0 / O tratamento utilizando Radioterapia em Arco Modulado Volumétrico é a modalidade mais moderna de radioterapia conformacional de forma que, com superposição de vários campos, as distribuições de dose forneçam uma perfeita conformação ao tumor, diminuindo a probabilidade de complicações nos tecidos normais adjacentes. Nesse sentido, muitos esforços estão sendo investidos para melhorar a conformidade de distribuição de dose, bem como a integração de técnicas de imagem para rastreamento de tumores e correção de variações inter e intrafração. Para isso, um intenso acompanhamento da qualidade dos processos e um programa de garantia de qualidade são fundamentais para a segurança dos pacientes e o cumprimento da legislação vigente; além do uso de diferentes metodologias de dosimetria para inter comparação e validação dos resultados. Este trabalho tem por objetivo avaliar e comparar o desempenho dos dosímetros OSL de óxido de alumínio (Al2O3:C) fabricados pela Landauer Inc. com os fabricados pela Rexon&trade; na dosimetria de feixes clínicos de fótons de energias altas empregados em radioterapia com tratamento em arco modulado volumétrico (VMAT) utilizando diferentes objetos simuladores. Os dosímetros foram caracterizados para radiação gama do 60Co e para feixes clínicos de fótons de 6 MV típicos de tratamentos por VMAT em condições de equilíbrio eletrônico e de dose máxima respectivamente. Testes de desempenho das leitoras TL e OSL utilizadas e repetibilidade das amostras foram avaliadas. Após realizados todos os testes, os dosímetros foram irradiados na simulação de diferentes tratamentos radioterápicos por VMAT e suas respostas comparadas ao sistema de planejamento. Todos os tipos de dosímetros apresentaram resultados satisfatórios na verificação das doses desse tipo de simulação de planejamento. Os dosímetros de Al2O3:C apresentaram resultados compatíveis entre si e validados pelos outros dosímetros e câmara de ionização. Em relação a melhor técnica, o sistema comercial OSL InLight apresenta maior praticidade e versatilidade para uso e aplicação na rotina clínica. / Dissertação (Mestrado em Tecnologia Nuclear) / IPEN/D / Instituto de Pesquisas Energéticas e Nucleares - IPEN-CNEN/SP

Dans de nombreux systèmes de traitement de l'information, le signal est numérisé, traité informatiquement, puis reconverti dans le domaine analogique. La faible bande passante de ces étapes de conversion numérique/analogique limite considérablement le débit d'informations traitées. Une solution purement analogique améliorerait donc considérablement le temps de traitement et la bande passante. Notre approche consiste à transférer le signal RF à traiter sur une porteuse optique puis à procéder à son traitement dans le domaine optique. L'étape de traitement est assurée par la traversée d'un cristal dopé en ions terres rares convenablement "programmé". Cette étape de programmation consiste à graver dans le profil d'absorption du cristal une fonction caractéristique de l'opération de traitement du signal à réaliser. Deux opérations ont ainsi été implémentées : 1) le renversement temporel de signaux RF : c'est l'opération consistant à générer analogiquement le signal renversé temporellement s(−t) d'un signal incident s(t). La fonction à graver dans le profil d'un cristal d'Er:YSO est alors un réseau spectral de pas variable. 2) l'analyse spectrale large bande instantanée : c'est l'opération permettant d'accéder au contenu spectral d'un signal. On impose au protocole de fournir instantanément le spectre d'un signal large bande. La fonction à graver dans le profil d'un cristal de Tm:YAG est alors un réseau spectro-spatial de pas variable. / Many signal processing devices rely on the digitalization of the incoming signal. After being processed by a computer, the signal needs to be converted back to its original analog form. Due to the limited bandwidth of analog-to-digital and digital-to-analog stages, the data flow rate is significantly limited. A purely analog solution would then significantly improve the processing time and bandwidth. In our approach, we first transfer the incoming RF signal on an optical carrier, allowing us to process it in the optical domain. For the processing stage, we propose to engrave the absorption profile of a rare earth ion-doped crystal with different shapes (each shape is specific to one processing operation). In this work, two operations are implemented: 1) time reversal of RF signals: we analogically generate the time reversed replica s(−t) of an incoming signal s(t). For this purpose, the shape to be engraved in the absorption profile of a Er:YSO crystal is a non-periodic spectral grating. 2) instantanous broadband spectral analysis: we want to instantaneously access the spectral components of a broadband signal. For this purpose, the shape to be engraved in the absorption profile of a Tm:YAG crystal is a spectro-spatial grating with a variable period.

Produkce hyperpolarizovaných plynů, především helia (3He) nebo xenonu (129Xe), nachází stále rostoucí rozsah aplikací v zobrazování magnetickou rezonancí (MRI). Helium ani xenon nejsou obyčejně obsaženy v těle a experimenty tedy nejsou ovlivněny nechtěným signálem z okolních tkání. Ukázalo se, že několika hyperpolarizačními technikami může být magnetická polarizace (magnetizace) jader vzácných plynů zvýšena na hladinu, se kterou jsou praktické aplikace proveditelné. Hyperpolarizované plyny mohou tedy být užitečným nástrojem pro neinvazivní zkoumání lidského dýchání, dovolující statické zobrazování během zadržení dechu nebo zkoumání dynamiky výdechu nebo nádechu, nebo funkčního zobrazování. V neživé přírodě, mohou být hyperpolarizovaný plyny využity jako kontrastní látka při studiu mikroporézních materiálů, jako jsou zeolity, stavební látky a hmoty, atd. V této doktorské práci je popsán vývoj a konstrukce aparatury pro hyperpolarizaci xenonu (izotopu 129Xe). Nákup hyperpolarizovaného xenonu od jiných výzkumných center v zahraničí a jeho dovážení by ovšem nebylo efektivní a to zejména z důvodu náročnosti zajištění potřebných fyzikálních podmínek pro přepravu hyperpolarizovaného plynu. Toto bylo hlavní motivací k vývoji vlastní technologie pro přípravu hyperpolarizovaného xenonu. Se zvládnutou technologií by bylo možné navázat spolupráci s medicínskými zařízeními, nebo s týmy zabývající se živou nebo neživou přírodou (např. při studiu mikroporézních materiálů, gelů, v zemědělských aplikacích nebo při výzkumu využívajících zvířat, atd.). Cílem této práce je studium teorie hyperpolarizovaných vzácných plynů se zaměřením na 129Xe a experimentální ověření a změření relaxačních časů pomocí jaderné magnetické rezonance. Vzhledem k tomu, že je možné hyperpolarizované vzácné plyny skladovat pro pozdější využití, se tato práce také zabývá možnostmi zásobníku hyperpolarizovaného vzácného plynu a jeho teoretickým a experimentálním řešením. V této práci jsou popsány především dva základní typy experimentů přípravy hyperpolarizovaného xenonu. V obou jsou využity zatavené válcové skleněné vzorky naplněné xenonem a doplňujícím plynem – dusíkem, heliem. První z experimentů se zabývá měřením vlastností termálně polarizovaného xenonu a druhý měřením vlastností hyperpolarizovaného xenonu. Pro hyperpolarizaci 129Xe bylo použito výkonového laseru a experimentálně byla zkoumána jednak míra polarizace na základě změny spektrální hustoty čerpacího laserového svazku a dále pak optimální doba optického čerpání 129Xe a relaxační časy xenonu.