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L'encéphalopathie associée au sepsis (EAS) est définie comme un dysfonctionnement cérébral diffus induit par une réponse systémique à une infection. Chez les patients septiques, l'imagerie par résonance magnétique (IRM) a indiqué à la fois des anomalies de la substance grise (SG) et blanche (SB) associées à des troubles cognitifs graves, y compris le delirium. Pour améliorer notre compréhension des changements hémodynamiques, métaboliques et structuraux associés au sepsis, différentes séquences d'IRM ont été réalisées chez des rats ayant subi une injection ip de solution saline ou de lipopolysaccharide bactérien (LPS) 2,5h plus tôt ou une ligature et ponction caecale 24h plus tôt. Après ip LPS, l'IRM de contraste de phase a été réalisée pour étudier le flux des artères cérébrales antérieures et moyennes et le marquage des spins artériels (ASL) pour étudier la perfusion des structures cérébrales de la SB et SG. Des séquences d'imagerie par diffusion pondérée (DWI) ont été utilisées pour évaluer les changements structurels. Après la chirurgie CLP, ASL a été utilisé pour étudier les changements de la microcirculation. L'imagerie pondérée en T2, l'imagerie du tenseur de diffusion (DTI) et les statistiques spatiales basées sur les faisceaux (TBSS) ont été réalisées pour caractériser les événements structurels dans différentes structures cérébrales. Après imagerie, les animaux ont été sacrifiés et leur cerveau a été traité pour l'histologie afin de détecter l'enzyme synthétisant les prostaglandines vasoactives cyclooxygénase-2 (COX-2) et le canal hydrique astrocytaire aquaporin-4 (AQP4) dont l'expression peut être régulée à la hausse, évaluer la présence d'immunoglobulines périvasculaires (Ig) indiquant une rupture de la barrière hémato-encéphalique (BHE) et étudier la morphologie des glies puisque la microglie et l’astroglie changent de morphologie lors des conditions inflammatoires. L'IRM n'a indiqué aucun changement hémodynamique dans la substance grise après l'administration de ip LPS, alors qu'une perfusion cérébrale accrue a été montrée au niveau du corps calleux comme indiqué par l'ASL. DTI a indiqué une augmentation de la diffusion des molécules d’eau parallèlement aux fibres du corps calleux. Ces changements étaient accompagnés d'une dégradation de BHE dans la SB ainsi que la substance grise corticale et striatale adjacente tel est indiqué par la présence périvasculaire d'IgG, sans aucun changement majeur de COX-2 vasculaire ou de morphologie des glies du coprs calleux. Le dysfonctionnement du SNC induit par le sepsis a résulté en une augmentation du contraste pondéré en T2 dans le cortex, le striatum et la base du cerveau, une diminution de la perfusion sanguine dans le cortex et une augmentation de la diffusion hydrique du corps calleux et du striatum ventral. Ces changements ont été associés dans la SB à des modifications de la morphologie des glies et dans la substance grise à une expression constitutive de COX-2 et AQP4 plus faible dans le cortex cérébral. La comparaison entre CLP ayant subit ou non une IRM sous anesthésie à l'isoflurane a montré une réponse inflammatoire réduite tel est indiqué par l'expression de COX- 2, une activation réduite des glies ainsi qu’une lésion réduite de la BHE dans le CLP subissant une IRM sous anesthésie. Collectivement, nos résultats suggèrent que des changements hémodynamiques peuvent survenir en l'absence de flux altéré dans les artères irriguant le cerveau antérieur. Ensuite, l'altération de la structure de la SB est une étape précoce de la pathogenèse de l’EAS qui peut résulter soit de la dégradation de la BHE, soit de l'activation des glies. Cette étude sous-tend l'effet délétère d'une seule exposition à l'anesthésie à l'isoflurane qui peut être atténuée par une seconde exposition chez les rats ayant subi une laparotomie ainsi que les effets de l'inflammation systémique induite par le CLP sur les glies pouvant être atténués par imagerie sous anesthésie à l'isoflurane. / Sepsis-associated encephalopathy (SAE) refers to central nervous system dysfunction during the systemic inflammatory response to infection. In septic patients with encephalopathy MRI has indicated both gray and white matter abnormalities that were associated with worse cognitive outcome including delirium. To improve our understanding of sepsis-associated hemodynamic, metabolic, and structural changes, different MRI sequences were performed in rats that either underwent an i.p injection of saline or bacterial lipopolysaccharide (LPS) 2.5h earlier or cecal ligation and puncture (CLP) 24h earlier. After ip LPS, phase contrast MRI was performed to study anterior and middle cerebral arteries flow and Arterial Spin Labeling (ASL) to study perfusion of white and grey matter brain structures. Diffusion Weighted Imaging (DWI) sequences was used to assess structural changes. After CLP surgery, ASL was used to study microcirculation changes. T2-Weighted Imaging, Diffusion Tensor Imaging (DTI) and tract-based spatial statistics (TBSS) were performed to characterize structural events in different brain structures. After imaging, animals were sacrificed and their brains processed for histology to detect the vasoactive prostaglandin-synthesizing enzyme cyclooxygenase-2 (COX-2) and the astrocytic aquaporin-4 water channel (AQP4) the expression of which can be upregulated during inflammation, to assess the presence of perivascular immunoglobulins (Ig) indicating blood-brain barrier (BBB) leakage and to study glia cell morphology as both microglia and astrocytes are known to change their morphology in inflammatory conditions. Magnetic resonance rat brain imaging indicated no hemodynamic changes in the grey matter after ip LPS administration while an increased CBF was shown in corpus callosum white matter as indicated by ASL. DTI indicated increased water diffusion parallel to fibers of the corpus callosum white matter. These changes were accompanied by BBB breakdown in the white matter and adjacent cortical and striatal grey matter as indicated by the perivascular presence of IgG, but no major changes in vascular COX-2 or white matter glia cell morphology. CLP induced sepsis-associated CNS dysfunction resulted in higher T2-weighted contrast intensities in the cortex, striatum and base of the brain, decreased blood perfusion distribution to the cortex and increased water diffusion in the corpus callosum and ventral striatum compared to sham surgery. These changes were associated in the white matter with modifications in glia cells morphology and in the grey matter with lower expression of constitutive COX-2 expression and AQP4 in the cerebral cortex. The comparison between CLP that underwent or not MRI under isoflurane anesthesia indicated reduced inflammatory response as indicated by COX-2 expression, reduced glia activation and reduced BBB damage in CLP that underwent MRI under isoflurane anesthesia. Collectively, our results suggest that hemodynamic changes may occur in the absence of altered flow in forebrain irrigating arteries. Then, altered white matter structure is an early step in SAE pathogenesis that may result either from BBB breakdown or glial cells activation. This study underlies the deleterious effects of a single exposure to isoflurane anesthesia that may be mitigated by a second exposure in sham-operated rats and the effects of CLP-induced systemic inflammation on glial cells that can be attenuated by imaging under isoflurane anesthesia.

This dissertation consist of three parts. The first part of the thesis is devoted to the study of gravity and higher spin gauge theories in 2+1 dimensions. We construct cosmological so-lutions of higher spin gravity in 2+1 dimensional de Sitter space. We show that a consistent thermodynamics can be obtained for their horizons by demanding appropriate holonomy conditions. This is equivalent to demanding the integrability of the Euclidean boundary CFT partition function, and reduces to Gibbons-Hawking thermodynamics in the spin-2 case. By using a prescription of Maldacena, we relate the thermodynamics of these solutions to those of higher spin black holes in AdS3. For the case of negative cosmological constant we show that interpreting the inverse AdS3 radius 1=l as a Grassmann variable results in a formal map from gravity in AdS3 to gravity in flat space. The underlying reason for this is the fact that ISO(2,1) is the Inonu-Wigner contraction of SO(2,2). We show how this works for the Chern-Simons actions, demonstrate how the general (Banados) solution in AdS3 maps to the general flat space solution, and how the Killing vectors, charges and the Virasoro algebra in the Brown-Henneaux case map to the corresponding quantities in the BMS3 case. Our results straightforwardly generalize to the higher spin case: the flat space higher spin theories emerge automatically in this approach from their AdS counterparts. We also demonstrate the power of our approach by doing singularity resolution in the BMS gauge as an application. Finally, we construct a candidate for the most general chiral higher spin theory with AdS3 boundary conditions. In the Chern-Simons language, the left-moving solution has Drinfeld-Sokolov reduced form, but on the right-moving solution all charges and chemical potentials are turned on. Altogether (for the spin-3 case) these are 19 functions. Despite this, we show that the resulting metric has the form of the “most general” AdS3 boundary conditions discussed by Grumiller and Riegler. The asymptotic symmetry algebra is a product of a W3 algebra on the left and an affine sl(3)k current algebra on the right, as desired. The metric and higher spin fields depend on all the 19 functions. The second part is devoted to the problem of Neumann boundary condition in Einstein’s gravity. The Gibbons-Hawking-York (GHY) boundary term makes the Dirichlet problem for gravity well defined, but no such general term seems to be known for Neumann boundary conditions. In our work, we view Neumann boundary condition not as fixing the normal derivative of the metric (“velocity”) at the boundary, but as fixing the functional derivative of the action with respect to the boundary metric (“momentum”). This leads directly to a new boundary term for gravity: the trace of the extrinsic curvature with a specific dimension-dependent coefficient. In three dimensions this boundary term reduces to a “one-half” GHY term noted in the literature previously, and we observe that our action translates precisely to the Chern-Simons action with no extra boundary terms. In four dimensions the boundary term vanishes, giving a natural Neumann interpretation to the standard Einstein-Hilbert action without boundary terms. We also argue that a natural boundary condition for gravity in asymptotically AdS spaces is to hold the renormalized boundary stress tensor density fixed, instead of the boundary metric. This leads to a well-defined variational problem, as well as new counter-terms and a finite on-shell action. We elaborate this in various (even and odd) dimensions in the language of holographic renormalization. Even though the form of the new renormalized action is distinct from the standard one, once the cut-off is taken to infinity, their values on classical solutions coincide when the trace anomaly vanishes. For AdS4, we compute the ADM form of this renormalized action and show in detail how the correct thermodynamics of Kerr-AdS black holes emerge. We comment on the possibility of a consistent quantization with our boundary conditions when the boundary is dynamical, and make a connection to the results of Compere and Marolf. The difference between our approach and microcanonical-like ensembles in standard AdS/CFT is emphasized. In the third part of the dissertation, we use the recently developed CFT techniques of Rychkov and Tan to compute anomalous dimensions in the O(N) Gross-Neveu model in d = 2 + dimensions. To do this, we extend the “cow-pie contraction” algorithm of Basu and Krishnan to theories with fermions. Our results match perfectly with Feynman diagram computations.

Usando uma transformação de dualidade generalizada, considerações de simetria e supondo que as superfície críticas sejam contínuas, obtivemos o dia grama de fase para sistemas de spins Z (N) bidimensionais e sistemas com invariança de calibre Z (N) a quatro dimensões. Caracterizamos as diversas fases dos sistemas de spins pelo valor esperado das potências dos operadores de ordem e desordem. No sistema com invariança de calibre, por outro lado, estas fases caracterizadas pelo comportamento do valor esperado das potências das alças de Wilson e de \'t Hooft. Obtivemos para ambos os sistemas fases moles em que no caso de spins 2D (calibre 4D) todas as potências dos parâmetros de ordem e desordem ( todas as potências das alças de Wilson e \'t Hooft) são nulas (exibem decaimento com o perímetro da alça). Enquanto no sistema com invariança de calibre todas as combinações de decaimento (área ou perímetro) das alças de Wilson e \'t Hooft são permitidas, as relações de comutação no sistema de spins proíbe a existência de fases em que tanto o parâmetro de ordem como o de desordem são não nulos (exceto quando estes operadores comutam). Apresentamos por completeza as relações de dualidade para sistemas de calibre Z (N) com campos de Higgs a três dimensões. / Using a generalized duality transformation, symetry considerations and assuming that criticality is continuous in the system?s parameters, we obtain the phase diagram for two-dimensional Z (N) spins system?s and four-dimensional gauge Z (N) system\'s. For spins system we characterize the various phases by the expectation value of powers of the order and disorder operators. For gauge systems, on the other hand, the characterization is via decay law of powers of Wilson and \'t Hooft loops. We obtain soft phases for both systems, with the folowing, behaviour: for spins system all powers of order and disorder parameters vanish, whereas for gauge systems all powers of Wilson and \'t Hooft loops decay like the perimeter. Whereas all combinations of area and perimeter decay are allowed for Wilson\'s and \'t Hooft\'s loops, the Z (N) commutation relations for spin systems forbid the simultaneous non-vanishing of order and disorder parameters (except when these operators commute). For completeness we include the duality relations for three-dimensional gauge plus Higgs Z(N) systems.

Submitted by Fabio Sobreira Campos da Costa (fabio.sobreira@ufpe.br) on 2016-06-29T13:52:59Z No. of bitstreams: 2 license_rdf: 1232 bytes, checksum: 66e71c371cc565284e70f40736c94386 (MD5) tese_final.pdf: 5635071 bytes, checksum: b300efb627e9ece412ad5936ab67e8e2 (MD5) / Made available in DSpace on 2016-06-29T13:52:59Z (GMT). No. of bitstreams: 2 license_rdf: 1232 bytes, checksum: 66e71c371cc565284e70f40736c94386 (MD5) tese_final.pdf: 5635071 bytes, checksum: b300efb627e9ece412ad5936ab67e8e2 (MD5) Previous issue date: 2013-08-26 / CNPq / No presente trabalho duas classes de problemas são abordadas. Primeiramente, são apresentados estudos computacionais sobre o modelo O(n) de spins na rede quadrada, e em seguida apresentamos novas soluções exatas para a dinâmica de bolhas na célula de Hele-Shaw. O estudo do modelo O(n) é feito utilizando sua representação em laços (cadeias fechadas), a qual é obtida a partir de uma expansão para altas temperaturas. Nesse representação, a função de partição do modelo possui uma expansão diagramática em que cada termo depende do número e comprimento total de laços e do número de (auto)interseções entre esses laços. Propriedades críticas do modelo de laços O(n) são obtidas através de conceitos oriundos da teoria de percolação. Para executar as simulações Monte Carlo, usamos o eficiente algoritmo WORM, o qual realiza atualizações locais através do movimento da extremidade de uma cadeia aberta denominada de verme e não sofre com o problema de "critical slowing down". Para implementar esse algoritmo de forma eficiente para o modelo O(n) na rede quadrada, fazemos uso de um nova estrutura de dados conhecida como listas satélites. Apresentamos estimativas para o ponto crítico do modelo para vários valores de n no intervalo de 0 < n ≤ 2. Usamos as estatísticas de laços e vermes para extrair, respectivamente, os expoentes críticos térmicos e magnéticos do modelo. No estudo de dinâmica de interfaces, apresentamos uma solução exata bastante geral para um arranjo periódico de bolhas movendo-se com velocidade constante ao longo de uma célula de Hele-Shaw. Usando a periodicidade da solução, o domínio relevante do problema pode ser reduzido a uma célula unitária que contém uma única bolha. Nenhuma imposição de simetria sobre forma da bolha é feita, de modo que a solução é capaz de produzir bolhas completamente assimétricas. Nossa solução é obtida por métodos de transformações conformes entre domínios duplamente conexos, onde utilizamos a transformação de Schwarz-Christoffel generalizada para essa classe de domínios. / In this thesis two classes of problems are discussed. First, we present computational studies of the O(n) spin model on the square lattice and determine its critical properties, whereas in the second part of the thesis we present new exact solutions for bubble dynamics in a Hele-Shaw cell. The O(n) model is investigated by using its loop representation which is obtained from a high-temperature expansion of the original model. In this representation, the partition function admits an diagrammatic expansion in which each term depends on the number and total length of loops (closed graphs) as well as on the number of intersections between these loops. Critical properties of the O(n) model are obtained by employing concepts from percolation theory. To perform Monte Carlo simulations of the model, we use the WORM algorithm, which is an efficient algorithm that performs local updates through the motion of one of the ends (called head) of an open chain (called worm) and hence does not suffer from “critical slowing down”. To implement this algorithm efficiently for the O(n) model on the square lattice, we make use of a new data structure known as a satellite list. We present estimates for the critical point of the model for various values of n in the range 0 < n ≤ 2. We use the statistics about the loops and the worm to extract the thermal and magnetic critical exponents of the model, respectively. In our study about interface dynamics, we present a rather general exact solution for a periodic array of bubbles moving with constant velocity in a Hele-Shaw cell. Using the periodicity of the solution, the relevant domain of the problem can be reduced to a unit cell containing a single bubble. No symmetry requirement is imposed on the bubble shape, so that the solution is capable of generating completely asymmetrical bubbles. Our solution is obtained by using conformal mappings between doubly-connected domains and employing the generalized Schwarz-Christoffel formula for this class of domains.

Consideramos os efeitos de desordem ou aperiodicidade sobre três sistemas magnéticos distintos. Inicialmente, apresentamos um modelo fenomenológico para descrever a dependência térmica da magnetização remanente induzida por diluição numa classe de antiferromagnetos quase-unidimensionais. O modelo trata exatamente as correlações ao longo da direção dominante, levando em conta as demais interações por meio de um campo efetivo. Em seguida, utilizamos uma aproximação autoconsistente de Bethe-Peierls para avaliar os efeitos de um campo cristalino aleatório sobre os diagramas de fases de um modelo de Ising de spins mistos. Mostramos que a desordem é capaz de modificar a natureza dos pontos multicríticos existentes no limite uniforme do modelo. Finalmente, estudamos os efeitos de interações aleatórias ou aperiódicas sobre o comportamento da cadeia XX quântica em baixas temperaturas, através de câlculos numéricos baseados no mapeamento do sistema em um modelo de férmions livres. Apontamos evidências de que, em temperatura zero, existe um único ponto fixo universal, característico de uma fase de singleto aleatório, que governa o comportamento do modelo na presença de interações desordenadas. No caso de interações aperiódicas,obtemos resultados consistentes com previsões de grupo de renormalização, indicando, para uma certa classe de seqüências de substituição, um comportamento semelhante àquele associado à desordem. / We consider effects of disorder or aperiodicity on three different magnetic systems. First, we present a phenomenological model to describe the thermal dependence of the dilution-induced remanent magnetization in a class of quasi-one-dimensional antiferromagnets. The model treats correlations along the dominant direction in an exact way, while including the remaining inte-. i ractions via an effective field. Then, we use a self-consistent Bethe-Peierls ~ j .. approximation to gauge the effects of a random crystal field on the phase diagram of a mixed-spin Ising mode!. We show that disorder may have profound effects on the multicritical behavior associated with the uniform limit of the mo de!. Finally, we study effects of random or aperiodic interactions on the behavior of the quantum XX chain at low temperatures, by performing numerical calculations based on a mapping of the system onto a free-fermion mo de!. . We present evidence that, at zero temperature, there exists a single, universal fixed-point, associated with a random-singlet phase, which governs the behavior of the model in the presence of disordered interactions. In the case of aperiodic interactions, our results are consistent with renormalizationgroup predictions, indicating, for a certain class of substitution sequences, a behavior similar to the one induced by disorder.

On a compris ces dernières années que certaines mesures d'intrications sont un outil efficace pour la compréhension et la caractérisation de phases nouvelles et exotiques de la matière, en particulier lorsque les méthodes traditionnelles basées sur l'identification d'un paramètre d'ordre sont insuffisantes. Cette thèse porte sur l'étude de quelques systèmes quantiques à basse dimension où un telle approche s'avère fructueuse. Parmi ces mesures, l'entropie d'intrication, définie via une bipartition du système quantique, est probablement la plus populaire, surtout à une dimension. Celle-ci est habituellement très difficile à calculer en dimension supérieure, mais nous montrons ici que le calcul se simplifie drastiquement pour une classe particulière de fonctions d'ondes, nommées d'après Rokhsar et Kivelson. L'entropie d'intrication peut en effet s'exprimer comme une entropie de Shannon relative à la distribution de probabilité générée par les composantes de la fonction d'onde du fondamental d'un autre système quantique, cette fois-ci unidimensionnel. Cette réduction dimensionnelle nous permet d'étudier l'entropie aussi bien par des méthodes numériques (fermions libres, diagonalisations exactes, ...) qu'analytiques (théories conformes). Nous argumentons aussi que cette approche permet d'accéder facilement à certaines caractéristiques subtiles et universelles d'une fonction d'onde donnée en général.Une autre partie de cette thèse est consacrée aux trempes quantiques locales dans des systèmes critiques unidimensionnels. Nous insisterons particulièrement sur une quantité appelée écho de Loschmidt, qui est le recouvrement entre la fonction d'onde avant la trempe et la fonction d'onde à temps t après la trempe. En exploitant la commensurabilité du spectre de la théorie conforme, nous montrons que l'évolution temporelle doit être périodique, et peut même être souvent obtenue analytiquement. Inspiré par ces résultats, nous étudions aussi la contribution de fréquence nulle à l'écho de Loschmidt après la trempe. Celle-ci s'exprime comme un simple produit scalaire -- que nous nommons fidélité bipartie -- et est une quantité intéressante en elle-même. Malgré sa simplicité, son comportement se trouve être très similaire à celui de l'entropie d'intrication. Pour un système critique unidimensionnel en particulier, notre fidélité décroît algébriquement avec la taille du système, un comportement rappelant la célèbre catastrophe d'Anderson. L'exposant est universel et relié à la charge centrale de la théorie conforme sous-jacente. / In recent years, it has been understood that entanglement measures can be useful tools for the understanding and characterization of new and exotic phases of matter, especially when the study of order parameters alone proves insufficient. This thesis is devoted to the study of a few low-dimensional quantum systems where this is the case. Among these measures, the entanglement entropy, defined through a bipartition of the quantum system, has been perhaps one of the most heavily studied, especially in one dimension. Such a quantity is usually very difficult to compute in dimension larger than one, but we show that for a particular class of wave functions, named after Rokhsar and Kivelson, the entanglement entropy of an infinite cylinder cut into two parts simplifies considerably. It can be expressed as the Shannon entropy of the probability distribution resulting from the ground-state wave function of a one-dimensional quantum system. This dimensional reduction allows for a detailed numerical study (free fermion, exact diagonalizations, \ldots) as well as an analytic treatment, using conformal field theory (CFT) techniques. We also argue that this approach can give an easy access to some refined universal features of a given wave function in general.Another part of this thesis deals with the study of local quantum quenches in one-dimensional critical systems. The emphasis is put on the Loschmidt echo, the overlap between the wave function before the quench and the wave function at time t after the quench. Because of the commensurability of the CFT spectrum, the time evolution turns out to be periodic, and can be obtained analytically in various cases. Inspired by these results, we also study the zero-frequency contribution to the Loschmidt echo after such a quench. It can be expressed as a simple overlap -- which we name bipartite fidelity -- and can be studied in its own right. We show that despite its simple definition, it mimics the behavior of the entanglement entropy very well. In particular when the one-dimensional system is critical, this fidelity decays algebraically with the system size, reminiscent of Anderson's celebrated orthogonality catastrophe. The exponent is universal and related to the central charge of the underlying CFT.

Nous avons étudié, par RPE impulsionnelle, la cohérence quantique et des spins électroniques des ions de transition Mn2+, Co2+, Fe3+, et des complexes Fe3+/Cs+ et Fe3+/Na+, tous présents dans le ZnO monocristallin. Nous avons trouvé que l’anisotropie magnétique peut altérer la cohérence de la phase dynamique des qubits des spins électroniques. Nous avons mesuré une faible décohérence pour les spins d’ions Mn2+et Fe3+ dans ZnO, qui ont tous deux une faible anisotropie magnétique uniaxiale, tandis que les ions Co2+ isolés avec une très forte anisotropie magnétique uniaxiale, une décohérence rapide a été mis en évidence. Nous avons trouvé que les spins électroniques des complexes de type Fe3+/Cs+, ayant un tenseur d’anisotropie magnétique plus complexe que la simple anisotropie uniaxiale des ions Fe3+ isolés, possèdent presque le même temps de décohérence. Par la méthode des perturbations, nous avons mis en évidence théoriquement un terme supplémentaire à la phase habituelle de Berry, dû à l’anisotropie magnétique et qui existe dans tout système ayant un spin S>1/2. / We studied by pulsed EPR (p-EPR), the quantum coherence of electronic spins qubits of isolated transition metal ions of Mn2+, Co2+, Fe3+ and Fe3+/Cs+ as well as Fe3+/Na+ complexes, all found as traces in mono-crystalline ZnO. Indeed, we experimentally demonstrated that the magnetic anisotropy can alter the coherence of the dynamic phase of electronic spins qubits. We found a small decoherence for Mn2+ and Fe3+, spins having a small uniaxial magnetic anisotropy, and on the contrary, we found a very strong decoherence for Co2+ spins having a very strong uniaxial magnetic anisotropy. We found that the electronic spins of the Fe3+/Cs+ complex, having a more complex tensor magnetic anisotropy compared to the simplest uniaxial one of isolated Fe3+ spins in ZnO, have almost the same coherence time. By the perturbation method, we have found theoretically an additional term to the usual geometric Berry phase, due to the magnetic anisotropy which exists in any system having a spin S>1/2.

Nous analysons les caractéristiques d'intrication de quelques matériaux à l'état solide ainsi que des systèmes particuliers d'atomes et de champs en interaction. Une étude détaillée de la riche structure de phase des modèles de spins de basse dimension, décrivant le minéral naturel d'azurite et les composés de coordination à base de cuivre, a révélé des régimes à comportement d'intrication des plus robustes. En utilisant l'approche des systèmes dynamiques, la structure de phase de certains modèles classiques en réseaux hiérarchiques (récursifs) a aussi été étudiée et, pour la première fois, la transition entre régime chaotique et régime périodique au moyen de la bifurcation tangente a été détectée.Nous présentons une description détaillée des propriétés d'intrication de trois atomes piégés dans la limite dispersive. Une relativement simple accordabilité de la force atomique d'interaction de ce système et son étroite relation aux problèmes de frustration magnétique est démontrée. Les effets de propagation de pulses laser intenses dans un système atomique de type [lambda] avec des forces d'oscillateurs différentes sont analysés. Les résultats obtenus sont d'extrême importance dans des problèmes d'information quantique, comme par exemple, dans l'analyse du mécanisme de transfert de population dans des milieux ayant les propriétés définies ci-avant. Enfin, nous avons analysé les effets dissipatifs dans un protocole de distillation de l'intrication à variable continue récemment proposé. Malgré des contraintes additionnelles sur les paramètres du protocole, il est encore possible d'implémenter ce schéma de distillation évoqué ci-avant dans les technologies émergentes. / The entanglement features of some solid state materials, as well as of particular systems of interacting atoms and fields are analyzed. A detailed investigation of the rich phase structure of low dimensional spin models, describing the natural mineral azurite and copper based coordination compounds, has revealed regimes with the most robust entanglement behavior. Using the dynamical system approach, the phase structure of some classical models on hierarchical (recursive) lattices has been also studied and, for the first time, the transition between chaotic and periodic regimes by means of tangent bifurcation has been detected.A detailed description of entanglement properties of three atoms trapped in a cavity within the dispersive limit is presented. A relatively simple tunability of the atomic interaction strength of the above system and its close relation to the problems of frustrated magnetism is shown. Furthermore, the propagation effects of two intense laser pulses in a medium of [lambda] atoms with unequal oscillator strengths are investigated. Obtained results are crucial in some problems of quantum information theory, as, e.g., in the analysis of population transfer mechanism in media possessing the above properties. Finally, the dissipation effects in a recently proposed compact continuous-variable entanglement distillation protocol have been analyzed. Despite additional constraints on the parameters of the protocol, the discussed entanglement distillation scheme in quantum memories is still possible to implement within emerging technologies.

Cette thèse s’inscrit dans le cadre général de la théorie des systèmes intégrables avec bords et le développement des structures algébriques associées.D’une part, nous nous attaquons au problème de la diagonalisation de l’hamiltonien du modèle XXZ avec bords non diagonaux. Nous exhibons les deux ensembles d’états propres et valeurs propres du modèle si les paramètres de bords satisfont deux conditions.D’autre part, nous introduisons un modèle de physique statistique que nous appelons le modèle face avec un bord réfléchissant. Nous calculons exactement sa fonction de partition et nous montrons que cette dernière se représente simplement sous la forme d’un unique déterminant matriciel.Nous montrons que ces deux problèmes sont reliés par la transformation vertex-face et exhibent une structure algébrique commune, l’algèbre de réflexion dynamique. Nous nous intéressons aux aspects mathématiques de cette algèbre dans le cas elliptique général,et nous introduisons deux classes de ces représentations, la représentation de co-module d’évaluation et sa duale. Nous pensons que cette algèbre est la structure clef pour l’analyse des modèles faces avec bords. En particulier, nous montrons à l’aide de twists de Drinfel’d que leur fonction de partition se représente simplement dans le cas général. Enfin, nous tentons une ’dynamisation’ du modèle à vertex ’Half-Turn-Symmetric’,et nous décrivons sa fonction de partition en termes de représentation d’évaluation de l’algèbre de Yang-Baxter dynamique, et trouvons un ensemble de conditions la déterminantunivoquement. / This thesis is embedded in the general theory of quantum integrable models withboundaries, and the development of associated algebraic structures.We first consider the question of the diagonalization of the XXZ hamiltonian with nondiagonalboundaries. We succeed to find the two sets of eigenstates and eigenvalues of themodel if the boundaries parameters satisfy two conditions.We introduce then a statistical physics model which we refer to be the face model witha reflecting end. Moreover, we compute exactly its partition function and show that it takesthe form of a simple single matrix determinant.We show that these two problems are related through the vertex-face transformationand are solved using a common algebraic structure, the dynamical reflection algebra andits dual. We focus from a mathematical perspective on this algebra in the general ellipticcase. Both the co-module evaluation representation and its dual are introduced. We believethat these structures are the key ingredients for the analysis of face models with boundaries.In particular, using the concept of Drinfel’d twists, we show that the partition function ofthese models has a simple representation in the general case.Finally, we attempt on a ’dynamization’ of the Half-Turn-Symmetric vertexmodel. Wedescribe its partition function in terms of the evaluation representation of the dynamicalYang-Baxter algebra, and find a set of conditions that uniquely determine it.