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Cette thèse de doctorat vise l’examen critique de certaines théories de champ moyen nucléaire phénoménologiques, en se focalisant sur la description fiable des niveaux de particules individuelles. L’approche suivie ici est nouvelle en ce sens que elle permet non seulement la prédiction des valeurs numériques obtenues avec ce formalisme, mais également une estimation des distributions de probabilités correspondant aux résultats expérimentaux. Nous introduisons le concept des ≪erreurs théoriques≫, visant estimer, dans un cadre mathématique bien établi, les incertitudes relatives aux modélisations théoriques. Il est également introduit une notion subjective de pouvoir prédictif des Hamiltoniens nucléaires, qui est analysé dans le contexte des spectres énergétiques de particules individuelles. Le concept mathématique du ≪Problème Inverse≫ est appliqué aux Hamiltoniens de champ moyen réalistes. Cette technique permet la prédiction de propriétés du système partir d’un nombre limité de données. Afin d'approfondir notre connaissance des Problèmes Inverses, nous focalisons notre attention sur un problème mathématique simple. Une fonction dépendant de quatre paramètres libres est introduite afin de reproduire des données ≪expérimentales≫. Nous étudions le comportement des paramètres ≪fittés≫, leur corrélation, ainsi que les erreurs associées. Cette étude nous aide comprendre la signification de la formulation correcte du problème en question. Il nous montre également l'importance d'inclure les erreurs expérimentales et théoriques dans la solution. / This thesis is a critical examination of phenomenological nuclear mean field theories, focusing on reliable description of levels of individual particles. The approach presented here is new in the sense that it not only allows to predict the numerical values obtained with this formalism, but also yields an estimate of the probability distributions corresponding to the experimental results. We introduce the concept of ‘theoretical errors’ to estimate uncertainties in theoreticalmodels. We also introduce a subjective notion of ‘Predictive Power’ of nuclear Hamiltonians, which is analyzed in the context of the energy spectra of individual particles. The mathematical concept of ‘Inverse Problem’ is applied to a realistic mean-field Hamiltonian. This technique allows to predict the properties of a system from a limited number of data. To deepen our understanding of Inverse Problems, we focus on a simple mathematical problem. A function dependent on four free parameters is introduced in order to reproduce ‘experimental’ data. We study the behavior of the ‘fitted’ parameters, their correlation and the associated errors. This study helps us understand the importance of the correct formulation of the problem. It also shows the importance of including theoretical and experimental errors in the solution.

Dans une série de travaux Zied Ammari et Francis Nier ont développé des méthodes pour étudier la dynamique de champ moyen bosonique pour des états quantiques généraux pouvant présenter des corrélations. Ils ont obtenu des formules pour décrire la dynamique des corrélations, ou plus généralement des matrices densité réduites d'ordre arbitraire. Cette thématique a été largement développée ces dernières années. Norbert Mauser en a été un des contributeurs, ainsi que sur la notion de mesure de Wigner qui est la clé de l'analyse développée par Z. Ammari et F. Nier. En général, il est admis que l'asymptotique de champ moyen est une bonne approximation du problème à N particules quand N dépasse la dizaine. Cela concerne l'asymptotique de la matrice densité réduite à une particule qui ne décrit pas la dynamique des corrélations. Un objectif est de tester la validité de la dynamique de champ moyen pour les matrices densité réduites à 2-particules. Pour des tests numériques, les modèles discrets qui n'ont pas été vraiment traités en détail dans les travaux précédents de Z. Ammari et F. Nier semblent bien adaptés. La thèse comprendra donc plusieurs étapes: adapter les résultats précédents de Z. Ammari et F. Nier à des modèles discrets , développer des méthodes numériques pour des systèmes simples mais pertinents, permettant de valider l'approximation de champ moyen et les formules pour la dynamique des corrélations. Au niveau numérique, on utilise des schémas numériques symplectiques, développés spécifiquement ces dernières années pour la discrétisation des équations hamiltoniennes. Une dernière étape concerne la combinaison des deux asymptotiques, champ moyen et approximation des modèles continus par les modèles discrets. / In a serie of works Z. Ammari and F. Nier developed methods to study the dynamics of bosonic mean field for general quantum states which can present correlations. They obtained formulas to describe the dynamics of the correlations, or more generally reduced density matrices with an arbitrary order. This topic was widely developed these last years. N.J. Mauser was one of contributors, as well as on the notion of Wigner measure which is the key of the analysis developed by Z. Ammari and F. Nier. Generally, the mean field asymptotic is admitted is a good approximation of the N-body problem when N exceed about ten. It concerns the asymptotics of the reduced density matrices for one particle which does not describe the dynamics of the correlations. An objective is to test the validity of the mean field dynamics for reduced density matrices for 2 particles. For numerical tests, the discrete models which were not really handled in detail in the previous works of Z. Ammari and F. Nier seem adapted well. The thesis will thus include several steps: adapt the previous results from Z. Ammari and F. Nier to discrete models , develop numerical methods, for simple but relevant systems, allowing to validate the approximation of mean field and the formulas for the dynamics of the correlations. About numerics, symplectic numerical scheme are used, developed specifically these last years for the discretization of the hamiltonian equations. A last possible step concerns the combination of both asymptotics, that is mean field and approximation of the continuous models by the discrete models.

This master thesis is framed in the striking correspondence between gravity theories in Anti-de Sitter spacetime (AdS) and Conformal Field Theories (CFT). This is usually known as AdS/CFT duality and relates gravity theories in the bulk with CFTs that live in their conformal boundary. We start by presenting the notion of CFTs and some of the results and techniques that are widely used in this field. This includes conformal correlators for scalar and spin operators, the state-operator correspondence and the operator product expansion (OPE) of operators. The embedding formalism and the index-free notation to encode tensors in polynomials are also discussed and used throughout this work. The basic notions of AdS are outlined and CFT at finite temperature is then introduced. We include a review of thermal blocks and thermal coefficients for a thermal two-point function between scalar fields in mean field theory. We then analyse the thermal two-point function for conserved currents, which was not known in the literature. Finally, we start a study of its thermal blocks and thermal coefficients for the mean field theory application.

No description available.

Les symétries géométriques en usage en physique nucléaire sont assez peu variées, essentiellement la symétrie de l’ellipsoïde triaxial. On propose donc une méthode rigoureuse permettant d’étudier l’évolution et la possibilité de l’existence de symétries nouvelles dont la symétrie tétraédrique. Le formalisme de l’équation de SCHRÖDINGER est replacé dans le cadre des espaces de RIEMANN. Ce formalisme est utilisé dans le contexte du noyau de l’atome où l’on applique la théorie du champ moyen alliée à l’approximation adiabatique. Le noyau est le siège de deux catégories de mouvements adiabatiquement séparés, le mouvement rapide des nucléons dans le champ moyen, et le mouvement collectif modifiant lentement le champ moyen. Le second est régi par une équation de SCHRÖDINGER collective qui prend place dans un espace dont la métrique est donnée par le tenseur de masse. L’étude de la géométrie du noyau est alors calculable à l’aide de deux grands programmes développés dans le cadre de la thèse. / The geometrical symmetries used in nuclear physics are not very diversified, essentially the symmetry of the triaxial ellipsoid. One proposes therefore a rigourous method allowing to study the temporal evolution and the possibility of the existence of new symmetries among them the tetrahedral symmetry. The formalism of SCHRÖDINGER equation is reformulated in the framework of RIEMANN’s spaces. This formalism is used in the context of the atomic nucleus where one applies the mean-field theory combined with the adiabatic approximation. The nucleus is the terrain of two types of motions adiabatically separated, the quick motion of the nucleons in the mean-field and the collective motion modifying slowly the meanfield. The second one is governed by a collective SCHRÖDINGER equation written down in a space whose metric is given by the mass tensor. The study of the nucleus geometry is then computable with the help of two big programs developped within the thesis.

L'étude et la connaissance des propriétés électroniques des matériaux ne constituent pas seulement un enjeu technologique : il s'agit aussi d'un problème fondamental. Au delà des isolants et des métaux usuels, il existe des systèmes plus complexes dans lesquels même l'approximation du liquide de Fermi, pourtant fructueuse dans de nombreux cas, est mise en défaut par les fortes interactions.<br /><br />Le cas des premiers oxydes de métaux de transition, pour lesquels les orbitales de valence sont des orbitales 3d, est particulièrement intéressant. Le nombre quantique principal n = 3 est le plus faible autorisé pour la valeur l = 2 du nombre quantique angulaire : ainsi, étant déjà orthogonales aux autres orbitales par leur partie angulaire, les orbitales 3d n'ont pas besoin de noeuds dans leur partie radiale et sont donc assez localisées autour du noyau. La formation de bandes de conduction est possible (malgré le faible recouvrement direct entre orbitales 3d), mais en même temps les porteurs de charge sont soumis à de fortes interactions locales. A cause de ces corrélations, certains oxydes de métaux de transition (comme LaTiO3) sont isolants bien que leur bande 3d ne soit que partiellement remplie et qu'on attendrait donc une conductivité métallique. La localisation électronique peut aussi mener à la formation de moments magnétiques locaux, et l'interaction de ces derniers avec les porteurs de charge mobiles confère aux<br />Manganates leur propriété de magnéto-résistance géante. Enfin, on ne peut ne pas mentionner la célèbre famille des Cuprates CuO, pour lesquelles une supraconductivité haute Tc a été découverte en 1986.<br /><br />Parmi les oxydes de métaux de transition, les Cobaltates dopées au sodium NaxCoO2 suscitent elles aussi un grand intérêt. Leur fort pouvoir thermoélectrique associé à une faible résistivité suggère de possibles applications en réfrigération. Leur diagramme des phases fait apparaître la coexistence d'électrons de conduction et de moments magnétiques localisés, ainsi qu'une phase supraconductrice (ce sont donc les seuls oxydes de transition 3d supraconducteurs, avec les Cuprates et les Titanates). Comme dans les Cuprates, leur structure cristallographique est lamellaire et quasi-bidimensionnelle, mais contrairement à ces dernières où les Cu forment un réseau carré, les Co sont agencés en un réseau triangulaire susceptible de frustrer des interactions magnétiques. Malgré les nombreux travaux qui ont été consacrés à ces composés, la description de base de leur structure de bandes est sujette à controverse et les calculs “premiers principes” demeurent en désaccord avec les expériences de photoémission.<br /><br />Le travail présenté ici vise à obtenir un modèle effectif capable de prédire les bonnes excitations de basse énergie des Cobaltates de sodium. Après un chapitre d'introduction générale sur ces composés, j'exposerai les limites des calculs théoriques déjà effectués puis je décrirai la dérivation de notre modèle effectif avant de présenter les résultats obtenus. Des annexes seront<br />consacrées plus précisément aux méthodes théoriques discutées dans ce manuscrit.

We present a framework for learning in hidden Markov models with distributed state representations. Within this framework, we derive a learning algorithm based on the Expectation--Maximization (EM) procedure for maximum likelihood estimation. Analogous to the standard Baum-Welch update rules, the M-step of our algorithm is exact and can be solved analytically. However, due to the combinatorial nature of the hidden state representation, the exact E-step is intractable. A simple and tractable mean field approximation is derived. Empirical results on a set of problems suggest that both the mean field approximation and Gibbs sampling are viable alternatives to the computationally expensive exact algorithm.

A polymer is a large molecule constructed from many smaller structural units calledmonomers joined together by covalent bonds. Polymers have existed in natural formsince life began and those such as DNA, RNA, proteins and polysaccharides are someof the most important macromolecules found in plant and animal life. From the earliesttimes, the man has used many of these polymers as materials for providing clothing,decoration, tools, weapons and other requirements. However, the origins of today'spolymer industry commonly are accepted as being in the nineteenth century whenimportant discoveries were made concerning to the modification of certain naturalpolymers, as cellulose. The use of synthetic and natural polymers as stabilisers forcolloid systems (sols, dispersions, microemulsions, etc.) is becoming more importanteveryday in contemporary life. Polymer additives can be applied in preconcentrationsand dehydration of suspensions in mineral processing, purification of wastewater andeven in nutritional and pharmaceutical emulsions being their importance related to thecharacteristics of the process and the properties that they show. The present work aimsto develop appropriate numerical and analytical modelling techniques, which candescribe (considering the formation of loops and tails) the structure of a polymeric layeradsorbed on heterogeneous surfaces; this adsorbed layer is an relevant factor in theproperties showed by this kind of materials. Taking into account this, the methodologyknown as Single Chain Mean Field (SCMF) (originally used to study micellaraggregates and grafted polymers) was modified to apply on polymer adsorptionproblems. In this way, it was possible to calculate numerically properties that can beexperimentally measured, such as total monomer volume fraction profiles, loop and tailvolume fraction profiles, adsorbance or the thickness of the adsorbed layer. Thestructure of the polymeric layer was examined both for flat and spherical (colloidalparticles) surface geometries. When compared with other well establishedmethodologies for the numerical simulation of polymeric systems, this new version ofSCMF was found to be more efficient due to the improved sampling of the polymerchain configuration space.Thus, SCMF method results, in the case of the adsorption on flat surfaces, compare wellwith those obtained either with Monte Carlo simulations or with the method developedin the 80s by Scheutjens and Fleer (SCF). Due to the lack of studies focusing to polymeradsorption on colloidal particles, our results have been the first to present quantitativepredictions of the structure of the polymeric layer adsorbed on a spherical surface. Thus,we have demonstrated the dependence of the adsorbed polymer layer with the size ofthe colloidal particle as well as the characteristic lengths that influence on it. Finally, inthis work an analytical approach for the description of polymer-colloidal mixtures hasbeen developed which compares well with the numerical results obtained from theSCMF methodology. Furthermore, the analytical approach is able to predict systembehaviours, as for example the formation of gels. / Un polímero es una molécula de grandes dimensiones formada de pequeñas unidadesllamadas monómeros, los cuales se encuentran unidos por medio de enlaces covalentes.Los polímeros han existido de forma natural desde el comienzo de la vida, y aquelloscomo el DNA, RNA o las proteínas son algunos de los polímeros más importantesencontrados tanto en la vida animal como en la vegetal. Desde siempre el hombre hautilizado muchos de estos polímeros como materiales para hacer ropa, decoración,herramientas, etc. Sin embargo, el origen de la industria de polímeros que conocemoshoy en día se produjo en el siglo 19, gracias a importantes descubrimientos dentro de lamodificación de ciertos polímeros naturales, como la celulosa. El uso de polímerossintéticos y naturales como estabilizadores de sistemas coloidales (dispersiones,microemulsiones, etc.) juega en nuestros días un papel importante. Los polímerosutilizados como aditivos, pueden ser aplicados en preconcentraciones y deshidrataciónde suspensiones dentro de procesos minerales, tratamiento de aguas residuales e inclusolos podemos encontrar dentro de la industria farmacéutica y alimentaria, donde suimportancia es debida a la procesabilidad y propiedades que ellos exhiben. El trabajoque se presenta es orientado al desarrollo de técnicas de modelización, tanto analíticascomo computacionales, y su aplicación en la descripción (por medio de la formación debucles y colas) de la estructura de la capa de polímeros adsorbida en superficiesheterogéneas, siendo dicha capa de polímeros un factor importante en las propiedadesque este tipo de materiales presentan. Con este propósito, la metodología conocidacomo Single Chain Mean Field, utilizada anteriormente tanto para el estudio deagregados micelares como de polímeros anclados en superficies, ha sido modificadapara describir la adsorción de polímeros en superficies. Así se han podido calcularnuméricamente propiedades medibles experimentalmente como los perfiles de lafracción en volumen de monómeros totales, además de los pertenecientes a los bucles ycolas, adsorbancia o el espesor de la capa adsorbida, para geometrías de la superficieabsorbente tanto plana como esférica (partículas coloidales). En su comparación conotras metodologías, ya establecidas para la simulación numérica dentro de la física depolímeros, la aplicación de esta nueva versión del Single Chain Mean Field (SCMF)ha resultado ser más eficiente debido a un mejor muestreo del espacio deconfiguraciones de las cadenas poliméricas. De este modo, comparando los resultadosobtenidos a partir del SCMF, con aquellos obtenidos mediante técnicas de simulaciónMonte Carlo o la teoría desarrollada en los años 80 por Scheutjens y Fleer (SCF), se hapodido encontrar un buen acuerdo en las propiedades calculadas para el caso de laadsorción en superficies planas. Debido a la dificultad intrínseca del estudio de laadsorción en superficies curvadas, nuestros resultados son los primeros que presentanpredicciones cuantitativas sobre la estructura de la capa que se forma sobre unapartícula coloidal. Así hemos podido comprobar la dependencia de la estructura de lacapa de polímeros adsorbidos con el tamaño de la partícula sobre la que se encuentranadsorbidos además de las longitudes características de las cuales depende. Finalmente,en este trabajo se ha desarrollado, también, una teoría analítica para la descripción de lamezcla polímero-coloide. De este modo, los resultados numéricos obtenidos con elSCMF han podido ser comparados con dicha teoría, obteniendo, de nuevo, un buenacuerdo y predecir, además, comportamientos colectivos como la formación de geles.

From the time of the unexpected discovery of the insulating nature of NiO by Verwey half a century ago, Oxide materials have continued to occupy the centre stage of condensed matter physics. The recent discovery of high temperature superconductivity in doped cuprates has given a new impetus to the study of the strongly correlated electron systems. Besides, the occurrence of Colossal Magneto-Resistance (CMR) in doped rare earth manganite has also created renewed interest in these rather old systems. Understanding of the rich and complex phase diagram of these materials and their sensitivity to small perturbations e.g. external magnetic field of a few Tesla, temperature, change in isotope etc. are of great theoretical interest and also these materials have many potential technological applications. A common feature of all these oxide materials is that the transition metal ions have partially filled d-shells. Unlike s and p-electrons which gives rise to hybridized Bloch states, the d-electrons retain their atomic nature in a solid. This gives rise to strong Coulomb interaction among d-electrons which may be comparable or more than its kinetic energy. The strong correlation effects are evident from the experimental fact that the undoped parent compounds are insulators rather than metals as suggested by band theory, which favours a metallic state for systems with one electron per unit cell since this gives rise to partially filled bands (and hence a metallic state). These insulators termed Mott insulators, arise solely due to strong electron-electron correlations as compared to the band insulators which arise due to complete filling of one electron bands thereby giving rise to a gap (band gap)in the excitation spectra. The delicate competition between the kinetic energy and the Coulomb energy for d-electrons is broadly responsible for the wide variety of phenomena like Mott metal-insulator transition (MIT), magnetic transitions, charge ordering, orbital ordering, ferro/antiferroelectricity, and most interestingly the observation of high Tc superconductivity in doped cuprates. In this thesis we will restrict our interest to one such class of oxide materials, namely the doped rare earth manganites. In Chapter 1 we give a brief overview of the structure and basic interactions present in the doped manganites. Also, in the same Chapter we give a brief introduction to the phenomenology of manganites, particularly its phase diagram in the doping and temperature plane and various experimental features, e.g. the wide variety of phase transitions and phenomena particularly the observation of CMR, charge ordering and incipient meso-scale phase separations etc.. Then we briefly introduce a recently proposed microscopic model which is believed to be a minimal model which, for the first time, includes the three most important interactions present in the manganites namely the following -1)coupling of the orbitally degenerate eg electrons to local lattice distortions of Jahn-Teller type which gives rise to two species of electrons. The one denoted by by ℓ is associated with Jahn-Teller effects and hence is localized whereas the other denoted by b is an extended state and propagates through the lattice. 2) The strong Hund’s couplingof ℓ and b electrons to the t2g core spin and 3) the strong Coulomb correlation between the two species of electrons. Additionally, the model includes a new doping dependent ferromagnetic exchange between the t2g core spins which can arise from “virtual double exchange” mechanism which will be discussed in great detail in Chapter 1 . Finally, we give a brief account on Dynamical Mean Field Theory (DMFT) and Numerical Renormalization Group (NRG) as an impurity solver for the single impurity problem arising under single site DMFT approximation. In Chapter 2 we study the effect of inter-site ℓ - b hybridization on the ‘ℓ - b’ model. The single impurity problem arising under DMFT approximation has close connection with the Vigman-Finkelshtein (VF)model. Then we briefly introduce the VF model and bring out its close connection with the impurity problem. We consider both the particle-hole symmetric as well as the U → ∞ particle-hole asymmetric cases. We derive various spectral functions at T = 0K and discuss the nature of fixed points under various circumstances. We explicitly show that for the particle-hole symmetric case the Hamiltonian flows from X-ray edge singularity fixed point to Free Electron fixed point under Renormalization Group transformation. This is evident from the spectral properties of the model. We write down the effective Hamiltonian at the free electron fixed point. For the particle-hole asymmetric case the model flows from X-ray edge singularity fixed point to Free Electron/Strong Coupling fixed point with additional potential scattering terms. We write down the effective Hamiltonian at this fixed point and derive various leading order deviations. We found all of them to be irrelevant in nature also most interestingly the quasi-particles describing the under lying Fermi liquid state are found to be asymptotically non-interacting. We also calculate the Fermi liquid parameter, z, by analyzing the energy level structure of a non-interacting Hamiltonian with effective renormalized parameter. Also, we consider the case of ‘self consistent bath hybridization’ without ℓ - b hybridization for Bethe lattice with infinite coordination. Low energy qualitative features are found to be same but some of the high energy features get qualitatively modified. In Chapter 3 we discuss the transport properties of doped manganites in the insulating phases and also the Hall effect in the metallic phase. In the first part of this chapter we calculate the resistivity based on the ‘ℓ - b’model and try to fit it to the semiconducting form: ρ(T )= ρ0(T /T0)−nexp[Δ(T )/kBT ] and extract the “transport gap”, Δ(T ). This gap can be characterized in terms of the “spectral gap” which can be defined for the ℓ - b model. It is found that the transport gap in the paramagnetic phase can be characterized in terms of the near constant “spectral gap” in this phase whereas the same in the ferromagnetic phase can be characterized in terms of the zero temperature spectral gap. In the last part of this chapter we calculate the Hall resistivity (ρxy) of these materials in the metallic phase. Ρxy is found to be negative and linear in applied field -quite consistent with the experimental findings but this fails to explain the positive linear Hall resistivity at low temperatures and its crossover as a function of field and temperature. We then present a reasonable explanation for this discrepancy and support it by calculating the Hall density of states for a two band “toy model” involving inter species hybridization. In Chapter 4 we calculate the optical conductivity, σ(ω), in ℓ - b model. σ(ω) arises from two independent processes. One of the processes involves ‘b’ electrons only and termed as ‘b - b channel’ and this gives rise to a Drude peak in the low frequency region. another process termed as the ‘ℓ - b channel’ involves hopping of an ℓ-electron to a neighbouring empty site and transforms into a ‘b’like state. This process gives rise to a broad mid-infrared peak. The total conductivity is the sum of contributions from these two incoherent channels. Calculated σ(ω) for metallic systems shows lot of similarities with experimental observations particularly the temperature evolution of the mid-infrared peak and the spectral weight transfer between the two peaks. But for the insulating systems the calculated optical conductivity showed trends similar to more recent experimental observations on some insulating systems (x =0.125) but contradicts with earlier experimental observations on some other insulating system (x =0.1). Finally, in the concluding chapter, we summarize results from all the chapters and also sketch some possible future directions of investigations.