L’exploration de systèmes quantiques à N corps fortement corrélés représente l’un des domaines de recherche les plus stimulants de la physique contemporaine. Au cours des trente dernières années, les vapeurs diluées d’atomes neutres en suspension dans le vide et contrôlées par un laser sont devenues une plate-forme polyvalente et formidable pour l’étude de tels systèmes. L’intérêt principal réside dans la capacité d’ajuster arbitrairement la force de l’interaction atomique au moyen de résonances de Feshbach induites magnétiquement, ainsi que la possibilité de créer une large gamme de potentiels via des champs optiques précisément adaptés. Cette thèse présente les résultats récents de l’expérience FerMix, consacrée à l’étude des systèmes quantiques à plusieurs corps fermioniques à des températures ultra-basses utilisant les atomes alcalins 40K et 6Li. Les principaux résultats présentés dans ce texte sont doubles. Premièrement, nous rapportons la caractérisation expérimentale d’une nouvelle résonance de Feshbach (s,d)-wave du 40K, dont les résultats sont comparés aux prédictions théoriques correspondantes. En particulier, le spectre du taux de perte inélastique est déterminé pour différentes températures et profondeurs de piège, ce qui nous permet d’identifier les pertes en tant que processus à deux corps. De plus, il est confirmé que le canal d’entrée dominant est de type s-wave. À l’aide de modèles d’équation de taux, nous analysons le réchauffement observé de l’ensemble atomique et trouvons que le comportement est cohérent avec l’état lié prévu L = 2 présent dans le canal de sortie. Enfin, nous étudions expérimentalement la dynamique des populations de spin induite par les collisions inélastiques renforcées par résonance dans l’onde d, en observant un bon accord avec nos modèles numériques. En second lieu, nous résumons nos progrès dans l’étude des croisements dimensionnels entre le liquide de Tomonaga-Luttinger en 1D et le liquide de Landau-Fermi en 3D en utilisant les gaz de Fermi de 40K confinés dans un réseau optique à grand pas. Cela inclut à la fois les considérations de conception fondamentales et l’installation du matériel expérimental requis. / The exploration of strongly correlated quantum many-body systems represents one of the most challenging fields of research of contemporary physics. Over the past thirty years, dilute vapors of neutral atoms suspended in vacuum and controlled with laser light have become a versatile and powerful platform for the study of such systems. At the very heart lies the ability to arbitrarily tune the interaction strength by means of magnetically induced Feshbach resonances as well as the possibility to create a wide range of potential landscapes via precisely tailored optical fields. This thesis reports on the recent results of the FerMix experiment, which is dedicated to the study of fermionic quantum many-body-systems at ultralow temperatures using the Alkali atoms 40K and 6Li. The main results presented in this text are twofold. First, we report on the experimental characterization of a novel (s,d)-wave Feshbach resonance in 6Li, the results of which are compared to the corresponding theoretical predictions. In particular, the spectrum of the inelastic loss rate is determined for different temperatures and trap depths, which enables us to identify the losses as two-body processes. Moreover, the dominant entrance channel is confirmed to be s-wave in nature. Using rate equation models we analyze the observed heating of the atomic ensemble and find the behavior to be consistent with the predicted L = 2 bound state present in the exit channel. Finally, we investigate experimentally the dynamics of the spin populations driven by resonantly enhanced inelastic collisions in dwave, observing good agreement with our numerical models. Second, we summarize our progress towards the study of dimensional crossovers between the Tomonaga-Luttinger liquid in 1D and the Landau-Fermi liquid in 3D using Fermi gases of 40K confined in a large spacing optical lattice. This includes both the fundamental design considerations as well as the implementation of the required experimental hardware.

Dans cette thèse, nous avons exploré les possibilités de réaliser des structures hybrides à base graphène (GBHS) par la fonctionnalisation bilatérale du graphène. Le premier chapitre donne une introduction générale sur le graphène et sur la littérature concernant les différentes méthodes d’intercalations de métaux dans le graphène. Le chapitre 2 décrit les techniques expérimentales utilisées. Le chapitre 3 concerne la fonctionnalisation du graphène épitaxié sur SiC (0001) par intercalation d'atome d’or. Les différents modes d'intercalation de l’or ont été mis en évidence par microscopie tunnelle (formation d'agrégats d'atomes d'or individuels et formation d'une couche d'or continue). La nature de ces atomes d'or intercalées a été examinée par des calculs d’image de densité de charge, et par Spectroscopie de Photoélectrons X (XPS). La modification de la structure de bande du graphène a aussi été mise en évidence par Spectroscopie de Photoélectrons UV Résolue Angulairement (ARPES) par des expériences sur synchrotron. Ces études ont révélé une forte extension de la singularité de Van Hove et une augmentation de la vitesse de Fermi. Afin d’agir sur cette extension de la singularité de Van Hove, des molécules fortement donneuses d'électrons, telle que la molécule de TetraThioFulvalene (TTF) ont été déposée sur graphène intercalé or et sur graphite (chapitre 4). La dépendance du transfert de charge de ces molécules avec leur conformation et la réactivité photochromique de ces molécules conjuguées sur le graphène ont également été abordés. Pour comprendre les propriétés structurales de ces molécules, des mesures photophysiques ont été effectuées qui apparaissant dans le chapitre 5. / In this thesis, we have explored the possibilities to realize a Graphene Based Hybrid structures (GBHs) by the functionalization of a graphene layer on both sides. The first chapter gives a general introduction about graphene and a literature review of different metal intercalations on graphene. The second chapter explains the experimental techniques used in this work. In chapter 3, we studied the functionalization of epitaxial graphene on SiC(0001) by gold intercalation. With the help of Scanning Tunneling Microscopy, we have evidenced and characterized different intercalation modes such as the formation of aggregates of individual gold atoms and the formation of a continuous gold layer between the top graphene and the buffer layer. The free standing nature of the intercalated gold atoms was examined by differential charge density plot, projected density of states calculations and further by X-ray photoelectron spectroscopy. The band structure modification of graphene due to these intercalated gold atoms was evidenced by Angle-resolved photoemission spectroscopy, which reveals a strong Van Hove extension and an increase of the Fermi velocity. Extend to this research, to obtain an extended Van Hove singularity usually observed in highly doped graphene; we studied highly electron donor molecules, TetraThioFullvalene (TTF) on pristine and gold intercalated graphene and on graphite (chapter 4). The dependence of charge transfer of these molecules with their conformation and the reactivity of photochromic with conjugated molecules on graphene were also discussed. To understand the structural properties of these molecules photophysical measurements were performed in chapter 5.

The aim of this thesis was to find anomalies of elastic properties induced by topological changes of the Fermi surface. The latter are called "Lifshitz transitions". Lifshitz transitions are an interesting subject to study because a topological change of the Fermi surface results in a van Hove singularity of the density of states at the Fermi energy, which again induces an anomaly in the free energy and therefore yield anomalies of observable physical quantities. In all cases the question arose, if the corresponding van Hove singularities are large enough to cause anomalies in the elastic properties, which are measurable by nowadays experimental techniques and computable within the accuracy reachable in nowadays computer calculations. The calculations have been done with the Full-Potential nonorthogonal Local-Orbital minimum-basis band-structure code FPLO. To shift the van Hove singularities through the Fermi energy we used hydrostatic pressure, which is mimicked in the computations by decreasing the volume of the unit cell. The materials under consideration had been YCo5 and LaCo5 as examples for magnetic compounds and the element Osmium as an example for a non-magnetic material. All these materials exhibit hexagonal symmetry. In the case of YCo5 our calculations yield a first order Lifshitz transition. Here, an extraordinarily large peak in the spin-up part of the DOS, which is caused by a nearly dispersionless band in the hexagonal plane, crosses the Fermi level under a pressure of about 21 GPa. Thus, the spin-up 3d states become partly depopulated, which results in a drop of the total magnetic moment of 35%. Therefore the transition can be regarded as a transition from strong to weak ferromagnetism. Further, the transition results in a volume collapse of 1.4%. Though the volume collapse is isomorphic, it exhibits the following anisotropy: while the lattice constant in the hexagonal plane is almost smoothly contracting with increasing pressure, the lattice constant in c-direction collapses at the transition-pressure. This volume collapse has been verified in experiment. Analogous calculations have been performed for the compound LaCo5, which is isoelectronic to YCo5. Here as well we predict a first order Lifshitz transition, taking place at a pressure of about 23 GPa. The mechanism of the transition is the same than in YCo5. Again we find a volume collapse under pressure together with a decrease of the magnetic moment. The relative volume change amounts to 1.3%. Like in YCo5, the unit cell dimensions in the hexagonal plane are decreasing almost smoothly with pressure while in c-direction the lattice constant collapses at the transition-pressure. For LaCo5 there are no such experiments done so far to the best of our knowledge. For Osmium we found, that LDA reproduces the ground state volume very well. Furthermore, we could detect three Lifshitz transitions taking place at very high pressures of about 72 GPa, 81 GPa, and 122 GPa. At first, a hole ellipsoid appears at the Gamma-point (V=24.6Å^3, P=72 GPa), then a neck is created at the symmetry-line LH (V=24.2Å^3, P=81 GPa), and finally a hole ellipsoid appears at the L-point (V=23.2 Å^3, P=122 GPa). Due to a degeneracy in the band structure, the hole ellipsoid at the L-point appears at the same pressure when the necks, situated at the symmetry-lines LH merge at L. The corresponding van Hove singularities in the DOS are very tiny and thus no anomalies in the elastic properties could be detected. Furthermore, we showed that the kink in c/a at 25 GPa and at 27 GPa found by Occelli et al. [Occelli et al., Phys. Rev. Lett. 93, 095502 (2004)] and Ma et al. [Ma et al., Phys. Rev. B 72, 174103 (2005)], respectively, is not statistically significant and that (c/a)(P) can be fitted equally well by a smooth function as by piece-wise linear functions as proposed in these references. / Das Ziel dieser Arbeit war es, Anomalien in den elastischen Eigenschaften zu finden, die durch topologische Änderungen der Fermifläche - genannt "Lifschitz Übergänge" - hervorgerufen werden. Lifschitz Übergänge sind ein interessantes Forschungsgebiet, denn die topologische Änderung der Fermifläche führt zu einer van Hove Singularität in der Zustandsdichte, die an der Fermienergie liegt und eine Anomalie in der freien Energie hervorruft und deswegen zu Anomalien in beobachtbaren physikalischen Größen führt. In allen Fällen kam die Frage auf, ob die entsprechenden van Hove Singularitäten groß genug sind, um mit heutigen Methoden meßbare und berechenbare Anomalien in den elastischen Eigenschaften zu verursachen. Die Daten wurden mit dem Computerprogramm FPLO (Full-Potential nonorthogonal Local-Orbital minimum-basis band-structure scheme) berechnet. Um die van Hove Singularitäten durch die Fermienergie zu schieben, verkleinerten wir das Volumen der Einheitszelle, um hydrostatischen Druck zu simulieren. Als zu untersuchende Stoffe wurden YCo5 und LaCo5 als Beispiele für magnetische Verbindungen gewählt und Osmium als Beispiel für ein nicht magnetisches Element. Im Falle von YCo5 fanden wir einen Lifschitz Übergang erster Ordnung. Hier springt ein besonders großer Peak im Spin-auf Teil der Zustandsdichte unter einem Druck von ca. 21 GPa über die Fermienergie. Dadurch werden die Spin-auf 3d Zustände teilweise unbesetzt und das magnetische Moment verringert sich um 35%. Deswegen kann man den Übergang als einen Übergang von starkem Ferromagnetismus zu schwachem Ferromagnetismus bezeichnen. Das Volumen verkleinert sich hierbei um 1.4%. Obwohl dieser Volumenkollaps isomorph ist, zeigt er folgende Anisotropie: während die Gitterkonstante in der hexagonalen Ebene mit zunehmendem Druck mehr oder weniger glatt kontrahiert, kollabiert am Übergangsdruck die Gitterkonstante in c-Richtung. Dieser Volumenkollaps wurde vom Experiment verifiziert. Analoge Rechnungen wurden für die Verbindung LaCo5, die isoelektronisch zu YCo5 ist, durchgeführt. Auch hier sagen wir einen Lifschitz Übergang erster Ordnung voraus, der bei einem Druck von ca. 23 GPa stattfinden wird. Der Mechanismus dieses Übergangs ist der selbe wie in YCo5. Wiederum finden wir einen Volumenkollaps unter Druck zusammen mit einer Verringerung des magnetischen Moments. Die relative Volumenänderung beträgt hier 1.3%. Wie in YCo5 verläuft hier die Kontraktion der Gitterkonstante in der hexagonalen Ebene mehr oder weniger glatt, während die Gitterkonstante in c-Richtung am Übergang kollabiert. Für LaCo5 existieren unseres Wissens hierzu noch keine Experimente. Im Falle von Osmium fanden wir drei Lifschitz Übergänge bei sehr hohen Drücken von ca. 72 GPa, 81 GPa, und 122 GPa. Zuerst bildet sich ein Lochellipsoid am Gamma-Punkt (V=24.6Å^3, P=72 GPa), dann bildet sich ein Hals an der Symmetrielinie LH (V=24.2Å^3, P=81 GPa), und zum Schluß erscheint ein Lochellipsoid am L-Punkt (V=23.2 Å^3, P=122 GPa). Auf Grund einer Entartung in der Bandstruktur taucht das Lochellipsoid am L-Punkt an dem Druck auf, an dem sich auch die Hälse auf der Symmetrielinie LH bei L verbinden. Die entsprechenden van Hove Singularitäten in der Zustandsdichte sind jedoch extrem klein und deswegen können keine Anomalien in den elastischen Eigenschaften detektiert werden. Desweiteren zeigten wir, daß der Knick in c/a, den Occelli et al. [Occelli et al., Phys. Rev. Lett. 93, 095502 (2004)] bei 25 GPa und Ma et al. [Ma et al., Phys. Rev. B 72, 174103 (2005)] bei 27 GPa fanden, statistisch nicht relevant ist und daß (c/a)(P) genauso gut von einer glatten Funktion gefittet wird als von stückweise linearen Funktionen.

Η παρούσα εργασία αφορά στη μελέτη Χαμιλτώνιων συστημάτων Ν μη γραμμικών ταλαντωτών, όπως είναι αυτό των Fermi Pasta και Ulam (FPU), με στόχο την βαθύτερη κατανόηση της δυναμικής των σχεδόν-περιοδικών τροχιών και του ρόλου των αντίστοιχων τόρων στο χώρο φάσεων, καθώς αυξάνουμε την ενέργεια Ε και τον αριθμό βαθμών ελευθερίας Ν του συστήματος. Το βασικό μας αποτέλεσμα είναι ότι υπάρχουν τόροι χαμηλής διάστασης, που προκύπτουν από τη συνέχεια των αντίστοιχων του γραμμικού συστήματος, οι οποίοι ευθύνονται για τις FPU επαναλήψεις και εμποδίζουν την ισοκατανομή της ενέργειας μεταξύ όλων των κανονικών τρόπων ταλάντωσης. Αναλύοντας ευστάθεια αυτών των τόρων, μπορέσαμε να δώσουμε μια πληρέστερη ερμηνεία στο Παράδοξο των FPU, συνδέοντας και συμπληρώνοντας έτσι δύο από τις επικρατέστερες ερμηνείες του εν λόγω φαινομένου. / The present work concerns the study of Hamiltonian systems of N nonlinear coupled oscillators, as it is the one by Fermi Pasta and Ulam (FPU), in order to understand the dynamics of quasi-periodic orbits and the role of their corresponding tori in phase space, as we increase the energy E and the number N of the degrees of freedom. Our fundamental result is that there exist tori of low dimension, that come from the continuation of the corresponding tori of the linear system, which are responsible for the FPU recurrences and prevent the system from equipartition of the energy among all normal modes. By investigating the stability of these tori, we achieved to provide a more complete explanation for the FPU paradox, connecting and supplementing in this way two of the most dominant approaches for this paradox.

While the free electron model can often be surprisingly successful in describing properties of solids, there are plenty of materials in which interactions between electrons are too significant to be neglected. These strongly correlated systems sometimes exhibit rather unexpected, unusual and useful phenomena, understanding of which is one of the aims of condensed matter physics. Heat capacity measurements of paramagnetic YFe$_{2}$Ge$_{2}$ give a Sommerfeld coefficient of about 100 mJ mol$^{−1}$ K$^{−2}$, which is about an order of magnitude higher than the value predicted by band structure calculations. This suggests the existence of strong electronic correlations in the compound, potentially due to proximity to an antiferromagnetic quantum critical point (QCP). Existence of the latter is also indicated by the non-Fermi liquid T$^{3/2}$ behaviour of the low temperature resistivity. Below 1.8 K a superconducting phase develops in the material, making it a rare case of a non-pnictide and non-chalcogenide iron based superconductor with the 1-2-2 structure. This thesis describes growth and study of a new generation of high quality YFe$_{2}$Ge$_{2}$ samples with residual resistance ratios reaching 200. Measurements of resistivity, heat capacity and magnetic susceptibility confirm the intrinsic and bulk character of the superconductivity, which is also argued to be of an unconventional nature. In order to test the hypothesis of the nearby QCP, resistance measurements under high pressure of up to 35 kbar have been conducted. Pressure dependence of the critical temperature of the superconductivity has been found to be rather weak. μSR measurements have been performed, but provided limited information due to sample inhomogeneity resulting in a broad distribution of the critical temperature. While the superconductivity is the result of an effective attraction between electrons, under different circumstances the electronic properties of a system can instead be dictated by the Coulomb repulsion. This is the case for another transition metal based compound NiS$_{2}$, which is a Mott insulator. Applying hydrostatic pressure of about 30 kbar brings the material across the Mott metal-insulator transition (MIT) into the metallic phase. We have used the tunnel diode oscillator (TDO) technique to measure quantum oscillations in the metallised state of NiS$_{2}$, making it possible to track the evolution of the principal Fermi surface and the associated effective mass as a function of pressure. New results are presented which access a wider pressure range than previous studies and provide strong evidence that the effective carrier mass diverges close to the Mott MIT, as expected within the Brinkman-Rice scenario and predicted in dynamical mean field theory calculations. Quantum oscillations have been measured at pressures as close to the insulating phase as 33 kbar and as high as 97 kbar. In addition to providing a valuable insight into the mechanism of the Mott MIT, this study has also demonstrated the potential of the TDO technique for studying materials at high pressures.

L’alimentation en énergie des réseaux de capteurs miniaturisés pose une question fondamentale, dans la mesure où leur autonomie est un critère de qualité de plus en plus important pour l’utilisateur. C’est même une question cruciale lorsque ces réseaux visent à assurer une surveillance d’infrastructure (avionique, machines, bâtiments…) ou une surveillance médicale ou environnementale. Les matériaux piézoélectriques permettent d’exploiter l’énergie mécanique inutilisée présente en abondance dans l’environnement (vibrations, déformations liées à des mouvements ou à des flux d’air…). Ils peuvent ainsi contribuer à rendre ces capteurs autonomes en énergie. Sous la forme de nanofils (NF), les matériaux piézoélectriques offrent une sensibilité qui permet d’exploiter des sollicitations mécaniques très faibles. Ils sont également intégrables, éventuellement sur substrat souple.Dans cette thèse nous nous intéressons au potentiel des nanofils de matériaux semi-conducteurs piézoélectriques, tels que ZnO ou les composés III-V, pour la conversion d’énergie mécanique en énergie électrique. Depuis peu, ceux-ci ont fait l’objet d’études relativement nombreuses, avec la réalisation de nanogénérateurs (NG) prometteurs. De nombreuses questions subsistent toutefois avec, par exemple, des contradictions notables entre prédictions théoriques et observations expérimentales.Notre objectif est d’approfondir la compréhension des mécanismes physiques qui définissent la réponse piézoélectrique des NF semi-conducteurs et des NG associés. Le travail expérimental s’appuie sur la fabrication de générateurs de type VING (Vertical Integrated Nano Generators) et sur leur caractérisation. Pour cela, un système de caractérisation électromécanique a été construit pour évaluer les performances des NG réalisés et les effets thermiques sous une force compressive contrôlée. Le module d’Young et les coefficients piézoélectriques effectifs de NF de GaN; GaAs et ZnO et de NF à structure cœur/coquille à base de ZnO ont été évalués également dans un microscope à force atomique (AFM). Les nanofils de ZnO sont obtenus par croissance chimique en milieu liquide sur des substrats rigides (Si) ou flexibles (inox) puis sont intégrés pour former un générateur. La conception du dispositif VING s’est appuyée sur des simulations négligeant l’influence des porteurs libres, comme dans la plupart des études publiées. Nous avons ensuite approfondi le travail théorique en simulant le couplage complet entre les effets mécaniques, piézoélectriques et semi-conducteurs, et en tenant compte cette fois des porteurs libres. La prise en compte du piégeage du niveau de Fermi en surface nous permet de réconcilier observations théoriques et expérimentales. Nous proposons notamment une explication au fait que des effets de taille apparaissent expérimentalement pour des diamètres au moins 10 fois plus grands que les valeurs prévues par simulation ab-initio ou au fait que la réponse du VING est dissymétrique selon que le substrat sur lequel il est intégré est en flexion convexe ou concave. / Energy autonomy in small sensors networks is one of the key quality parameter for end-users. It’s even critical when addressing applications in structures health monitoring (avionics, machines, building…), or in medical or environmental monitoring applications. Piezoelectric materials make it possible to exploit the otherwise wasted mechanical energy which is abundant in our environment (e. g. from vibrations, deformations related to movements or air fluxes). Thus, they can contribute to the energy autonomy of those small sensors. In the form of nanowires (NWs), piezoelectric materials offer a high sensibility allowing very small mechanical deformations to be exploited. They are also easy to integrate, even on flexible substrates.In this PhD thesis, we studied the potential of semiconducting piezoelectric NWs, of ZnO or III-V compounds, for the conversion from mechanical to electrical energy. An increasing number of publications have recently bloomed about these nanostructures and promising nanogenerators (NGs) have been reported. However, many questions are still open with, for instance, contradictions that remain between theoretical predictions and experimental observations.Our objective is to better understand the physical mechanisms which rule the piezoelectric response of semiconducting NWs and of the associated NGs. The experimental work was based on the fabrication of VING (Vertical Integrated Nano Generators) devices and their characterization. An electromechanical characterization set-up was built to evaluate the performance and thermal effects of the fabricated NGs under controlled compressive forces. Atomic Force Microscopy (AFM) was also used to evaluate the Young modulus and the effective piezoelectric coefficients of GaN, GaAs and ZnO NWs, as well as of ZnO-based core/shell NWs. Among them, ZnO NWs were grown using chemical bath deposition over rigid (Si) or flexible (stainless steel) substrates and further integrated to build VING piezoelectric generators. The VING design was based on simulations which neglected the effect of free carriers, as done in most publications to date. This theoretical work was further improved by considering the complete coupling between mechanical, piezoelectric and semiconducting effects, including free carriers. By taking into account the surface Fermi level pinning, we were able to reconcile theoretical and experimental observations. In particular, we propose an explanation to the fact that size effects are experimentally observed for NWs with diameters 10 times higher than expected from ab-initio simulations, or the fact that VING response is non-symmetrical according to whether the substrate on which it is integrated is actuated with a convex or concave bending.

La théorie des spins élevés est le domaine de la physique théorique au centre de cette thèse. Le contexte général de la naissance de cette théorie est présentée dans l’introduction. La première partie est axée sur les ingrédients (méthode de Noether, fonctions génératrices et formalisme ambiant) permettant la construction de vertex cubiques entre un champ scalaire de matière et un champ de jauge de spin élevé dans un espace-temps à courbure constante à partir des courants conservés en espace-temps plat. Dans un second temps, nous préparons les éléments pour un futur test de la correspondance holographique à l’ordre cubique voire quartique en la constante de couplage. Plus précisément, nous révisons en détail le calcul de certains propagateurs, ce qui nous mène à calculer les fonctions à trois points impliquant deux scalaires. La dernière partie, bien que concernant toujours l’holographie des spins élevés, traite de la physique non-relativiste. Les symétries et les courants d’un gaz parfait/unitaire de Fermi y sont étudiés. Le lien entre physiques relativiste et non-relativiste est obtenue grâce à la réduction dimensionnelle de Bargmann. / The higher spin theory is the field of theoretical physics at the center of this thesis. The general context of the birth of this theory is presenting in the introduction. The first part focuses on the ingredients (Noether method, generating functions and ambient formalism) for the construction of cubic vertices between a scalar matter field and a higher spin gauge field in a constant curvature space-time from conserved currents in flat space-time. In a second step, we prepare the around for a future test of the holographic correspondence in the cubic or quartic order in the coupling constant. More specifically, we review in detail the computation of some propagators, which leads us to calculate three-point functions involving two scalars. The last part, although always on the higher spin holography, deals with non-relativistic physics. Symmetries and currents of an ideal or unitary Fermi gas are studied. The link between relativistic and non-relativistic physics is obtained by Bargmann dimensional reduction.

Submitted by Carlo Loria (santosloria@yahoo.com) on 2018-08-28T17:03:55Z No. of bitstreams: 1 TESE CARLO LORIA ALT.pdf: 11490877 bytes, checksum: d5002255e342591fc2e11a7b53ae7d92 (MD5) / Approved for entry into archive by NUBIA OLIVEIRA (nubia.marilia@ufba.br) on 2018-09-25T20:48:40Z (GMT) No. of bitstreams: 1 TESE CARLO LORIA ALT.pdf: 11490877 bytes, checksum: d5002255e342591fc2e11a7b53ae7d92 (MD5) / Made available in DSpace on 2018-09-25T20:48:40Z (GMT). No. of bitstreams: 1 TESE CARLO LORIA ALT.pdf: 11490877 bytes, checksum: d5002255e342591fc2e11a7b53ae7d92 (MD5) / CAPES / Na Itália, na passagem da década de 1960 para 1970, um quadro de fortes conflitos políticos nacionais repercutia sobre a vida universitária, sobre as pesquisas e ensejava profundas mudanças nas visões sobre a essência da ciência e sobre as práticas de investigação estabelecidas. O nível de radicalização gerou divergências e polarizações nas comunidades científicas, passando a ameaçar de cisão a Sociedade Italiana de Física, SIF. A ruptura não aconteceu graças à uma dinâmica endógena à própria comunidade que, mediante debates e propostas acadêmicas, encontrou a rota da pacificação. Esse processo tornou-se objeto de atenção de historiadores da ciência, interessados em explicar as condutas e protagonismos de membros da sociedade. As narrativas sugerem papeis importantes tanto das lideranças formais como das lideranças difusas, que emergiam de reuniões e assembleias, na proposição de temas para a Escola de Verão Enrico Fermi, que tinha lugar na cidade de Varenna. O objeto desta tese é tentar verificar como atuaram estas lideranças e se houve maior destaque ou supremacia de um tipo ou de outro. O campo de conhecimento desta pesquisa é a história da ciência com foco na comunidade de pesquisadores e o procedimento metodológico empregado privilegiou a utilização de fontes primárias como questionários aplicados à alguns informantes qualificados, pesquisadores da época, análise de epistolário entre esses pesquisadores e outras fontes como comunicações científicas. Os resultados esperados ajudarão a entender a solução da controvérsia. / ABSTRACT In Italy, during the sixties and seventies years of the las century, a series of strong national political riots and conflicts had an impact on university life, on research, and provoke deep changes on the views about the essence of science and established research practices. The level of radicalization has generated divergences and polarizations in the scientific communities, brought threats to split the Italian Physical Society, SIF. The rupture did not happen because to endogenous dynamics, inbuilt the own community, which, by means of debates and academic proposals, found the pacification route. This process attracted attention of historians of science, interested in explaining the conduct and protagonism of members of society. The narratives suggest important roles of both formal leaderships and diffuse leaderships, which emerged from meetings and assemblies, in proposing themes to the Enrico Fermi Summer School, which took place in the city of Varenna. The purpose of this thesis is to try to verify how these leaders acted and if there was greater prominence or supremacy from one type or another. The field of knowledge of this research is the history of science with a focus on the community of researchers and the methodological procedure employed privileged the use of primary sources as questionnaires applied to some qualified informants, researchers of the time, analysis of correspondence between these researchers and other sources as scientific communications. The expected results will help you understand the solution to the controversy.

Après plus d'un siècle d'étude des rayons cosmiques, des questions persistent à propos de leur origine. À l'échelle de notre galaxie, les vestiges de supernovæ sont d'excellents candidats en tant que sources de rayons cosmiques et il est aujourd'hui avéré que ces ondes de choc générées par l'explosion d'étoiles en fin de vie accélèrent des électrons jusqu'au TeV. Cependant, des preuves tangibles manquent toujours pour confirmer que les protons, qui représentent ~90% du rayonnement cosmique, y sont également accélérés. Ces preuves sont à chercher entre 100 MeV et 10 GeV où la forme spectrale de l'émission gamma nous renseigne sur la nature des particules accélérées.Ce domaine en énergie est observé par le satellite Fermi qui scrute le ciel à haute énergie grâce au Large Area Telescope (LAT), un instrument capable de détecter les rayons gamma d'énergies comprises entre 20 MeV et plus de 300 GeV. Avec la dernière version des données en date (Pass 8) rendue publique en 2015, la surface efficace a été sensiblement accrue, notamment à haute énergie. L'objet de cette thèse a été de mettre à profit les nouvelles performances du LAT pour étudier le rayonnement provenant de jeunes vestiges de supernovæ en coquille afin d'évaluer leur capacité à accélérer des particules à haute énergie. Au total, quatre vestiges de ce type ont été étudiés en détail : RCW 86, HESS J1731-347, SN 1006 et RX J1713.7-3946.L'analyse morphologique et spatiale de ces sources nous a menés à d'importants résultats : HESS J1731-347 et SN 1006 ont été détectés pour la première fois au GeV, nous avons mis en évidence une morphologie en coquille pour RCW 86 qui était précédemment détectée comme une source ponctuelle et RX J1713.7-3946 a révélé une forme spectrale plus complexe que ce qui était alors connu. Grâce à la modélisation de l'émission non-thermique de ces sources, en s'aidant des données au TeV obtenues par H.E.S.S., nous avons montré que leur émission gamma est très largement dominée par le rayonnement Compton inverse des électrons de haute énergie diffusant sur les champs de photons ambiants. Cependant, des modifications spectrales ont également été trouvées dans certaines parties de SN 1006 et RX J1713.7-3946 où l'onde de choc est en interaction avec des régions denses en matière, traçant la possible accélération de protons en leur sein. / After more than a century of cosmic-ray studies, questions about their origin remain unanswered. In our galaxy, supernova remnants are excellent candidates to be the sources of cosmic rays and it is now certain that these shock waves created by the explosion of dying stars accelerate electrons up to TeV energies. However, undeniable proof is still missing to confirm that protons, which represent ~90% of the cosmic radiation, are also accelerated. Such proof can be searched for between 100 MeV and 10 GeV, where the spectral shape of the gamma-ray emission changes according to the nature of the particles that are accelerated.This energy range is covered by the Fermi spacecraft which observes the high energy sky with the Large Area telescope (LAT), an instrument detecting gamma-rays from 20 MeV to more than 300 GeV. With the latest version of the data, released in 2015 (Pass 8), the effective area has been greatly improved, especially at high energy. The goal of this thesis was to take advantage of the improved performance of the LAT to study the radiation coming from young shell-type supernova remnants and to evaluate their ability to accelerate particles to high energy. Four such remnants were studied in detail: RCW 86, HESS J1731-347, SN 1006 and RX J1713.7-3946.Spatial and spectral analyses of these sources yielded important results: HESS J1731-347 and SN 1006 were identified for the first time in the GeV range, we detected a shell-like morphology for RCW 86 which was previously seen as a point source, and RX J1713.7-3946 revealed an unexpected spectral shape. Broadband modeling of the non-thermal emission of these remnants, using in particular TeV data obtained with H.E.S.S., showed that their gamma-ray emission is dominated by the inverse Compton scattering of electrons on ambient photon fields. However, we also found spectral modifications in some parts of SN 1006 and RX J1713.7-3946 where the shock is interacting with dense regions that could trace the acceleration of protons.

Submitted by Irene Nascimento (irene.kessia@ufpe.br) on 2017-04-17T18:48:07Z No. of bitstreams: 2 license_rdf: 1232 bytes, checksum: 66e71c371cc565284e70f40736c94386 (MD5) Dissertação Mestrado.pdf: 3421668 bytes, checksum: 4a6d6f2568841028e0b66b952f2d15ba (MD5) / Made available in DSpace on 2017-04-17T18:48:07Z (GMT). No. of bitstreams: 2 license_rdf: 1232 bytes, checksum: 66e71c371cc565284e70f40736c94386 (MD5) Dissertação Mestrado.pdf: 3421668 bytes, checksum: 4a6d6f2568841028e0b66b952f2d15ba (MD5) Previous issue date: 2016-08-30 / Este trabalho é uma extensão de uma modelagem tight−binding de estados de Wannier com interação coulombiana de screening para a descrição de elétrons correlacionados nas camadas de CuO2 do La2CuO4. Na condição de banda semicheia e temperatura T = 0 K, esta modelagem é capaz de predizer um estado fundamental antiferromagnético isolante e um estado excitado paramagnético com pseudo-gap, cuja natureza ainda é debatido na literatura. Esses estados são obtidos no contexto de uma solução auto-consistente tipo Hartree-Fock na modelagem de uma banda efetiva de estados de Wannier, sob condições de quebra de simetria de translações espaciais e efeito de emaranhamento (entanglement) na estrutura espinorial dos estados eletrônicos. No regime dopado com buracos, esses estados ficam degenerados num ponto crítico de concentração de buracos igual a xc = 0.2, resultando em uma transição de fase quântica de segunda ordem para um estado paramagnético. A modelagem dá assim explicação à existência detectada experimentalmente desta transição de fase. Em nosso trabalho generalizamos o termo cinético da modelagem acima mencionada através da inclusão de hopping entre segundos vizinhos, de acordo com observações experimentais. De fato, a inclusão deste novo termo cinético resulta em melhor concordância da previsão da modelagem e as observações experimentais da evolução da superfície de Fermi com dopagem de buracos. Em particular, enquanto na modelagem restrita a primeiros vizinhos não podemos conciliar a transição de fase quântica observada a xc = 0.2 com as características experimentais da evolução da superfície de Fermi, isto torna-se possível com a inclusão do hopping de segundos vizinhos com amplitude sugerida pelos resultados experimentais. / This work is an extension of a tight - binding model of states of Wannier with screened Coulomb interaction to the description of correlated electrons in the layers of CuO2 of the La2CuO4. In condition of half-filled band and temperature T = 0 K, this model is able to predict a antiferromagnetic insulating ground state and a paramagnetic excited state with pseudo-gap, which nature is still debated in the literature. These states are obtained in the context of a self-consistent solution type Hartree-Fock in the model of an effective band of the Wannier states under breaking conditions of symmetry of space translations and entanglement effect in the spinor structure of the electronic states. In scheme doped with holes, these states are degenerate at critical point of hole concentration equal to xc = 0.2, resulting in a quantum phase transition of second order to paramagnetic state. The model thus gives explanation to the existence of this experimentally detected phase transition. In our work we generalize the kinetic term of above mentioned model by inclusion of hopping between seconds neighboring, according to experimental observations. In fact, the inclusion of this new kinetic term results in better agreement of the forecast of the model and experimental observations of the evolution of the Fermi surface with holes doping. In particular, while the model is restricted to the first neighbors can not reconcile quantum phase transition observed at xc = 0.2 with the experimental characteristics of the evolution of the Fermi surface, this becomes possible with the inclusion of hopping between second neighboring with ampliude suggested by experimental results.