Made available in DSpace on 2014-06-11T19:25:30Z (GMT). No. of bitstreams: 0 Previous issue date: 2011-03-11Bitstream added on 2014-06-13T19:32:38Z : No. of bitstreams: 1 azevedo_tac_me_ift.pdf: 373974 bytes, checksum: 6a2336bc24ee4aed68e9d75a6f8dc9d1 (MD5) / Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES) / A correspondência AdS/CFT, da forma como foi conjecturada por Maldacena, sugere uma equivalência notável entre duas teorias aparentemente não relacionadas, quais sejam uma teoria de supercordas tipo IIB em um background AdS5 × S5 e uma teoria de super Yang–Mills (SYM) em quatro dimensões maximalmente supersimétrica(N = 4). Nesta dissertação, estudamos a relação entre o espectro da teoria de supergravidade tipo IIB em AdS5 × S5 (limite de baixas energias da teoria de supercordas mencionada acima) e a família de operadores invariantes degauge em N = 4 SYM descrita em [P. Howe, P. West, Int. J. Mod. Phys. A 14 (1999) 2659] através do uso de um superespaço harmônico, tendo como base principal o artigo [P. Heslop, P. Howe, Phys. Lett. B 502 (2001) 259]. Fazemos ainda uma revisão do formalismo de cosets, que é amplamente utilizado neste trabalho / The AdS/CFT correspondence, as conjectured by Maldacena, suggests a remarkable equivalence between two apparently unrelated theories, namely a type IIB superstring theory on an AdS5 ×S5 background and a maximally supersymmetric (N = 4) super Yang–Mills (SYM) theory in four dimensions. In this dissertation, we study the relation between the spectrum of the type IIB supergravity theory on AdS5 × S5 (low-energy limit of the superstring theory mentioned above) and the family of gauge-invariant operators inN = 4 SYM described in [P. Howe, P. West, Int. J. Mod. Phys. A 14 (1999) 2659] by making use of a harmonic superspace, mostly based on [P. Heslop, P. Howe, Phys. Lett.B502 (2001) 259]. Moreover, we review the coset space formalism, which is largely used in the present work

Este trabalho tem o objetivo de rever a obtenção das soluções do tipo brana em supergravidade e contém uma dedução detalhada das soluções extrema e negra. A fim de motivar algumas escolhas feitas ao longo do cálculo, o trabalho inclui uma breve revisão dos conceitos advindos da teoria de cordas e supersimetria. Esta revisão nos permitirá ainda relacionar as soluções da supergravidade com as branas da teoria de cordas e tecer considerações sobre o papel desta relação na dualidade entre teoria de calibre e gravitação. / This work intends to review the brane solutions of supergravity and contains a datailed deduction of the extremal and black solutions. In order to provide some motivations to the choices through the calculation, this work includes a brief review of some concepts from string theory and supersymmetry. This review will enable us to relate the supergravity solutions to string theory\'s branes and to make considerations about the role of this relationship in the duality between gauge and gravity theories.

This thesis is devoted to various questions connected with duality. It is composed of two parts.The first part discusses some aspects of timelike T-duality. We explore the possibility of compactification of supergravity theories with various signatures(low energy limit of M-theories which are dual under timelike T-dualities) on parallelizable internal seven dimensional (pseudo-)spheres. We show that, beside the standard theory, only one of the dual theories known as M'-theory can admit such a solution. The effective four dimensional theory is non-supersymmetric and due to the presence of torsion the symmetry of seven dimensional (pseudo-)sphere breaks down to Spin(3, 4). In the second part, in an attempt to have a systematic discussion of gaugings in supergravity, we show the isomorphism between the space of local deformations of the appropriate zero coupling limit of the embedding tensor Lagrangian and that of the second-order scalar-vector Lagrangian, describing the bosonic sector of supergravity ignoring gravity, in a chosen duality frame determined by embedding tensors. We analyze the BV-BRST deformation of a class of scalar-vector coupled Lagrangians, which contains supergravity Lagrangians as examples, and find a set of constraints that guarantee the consistency of the deformations of the Lagrangians. We show in principle that for a large class of theories considered in this thesis, the only deformations are those of the Yang-Mills type associated with a subgroup of the rigid symmetries. / Doctorat en Sciences / info:eu-repo/semantics/nonPublished

A lot of developments made during the last years show that Kac-Moody algebras play an important role in the algebraic structure of some supergravity theories. These algebras would generate infinite-dimensional symmetry groups. The possible existence of such symmetries have motivated the reformulation of these theories as non-linear sigma-models based on the Kac-Moody symmetry groups. Such models are constructed in terms of an infinite number of fields parametrizing the generators of the corresponding algebra. If these conjectured symmetries are indeed actual symmetries of certain supergravity theories, a meaningful question to elucidate will be the interpretation of this infinite tower of fields. Another substantial problem is to find the correspondence between the sigma-models, which are explicitly invariant under the conjectured symmetries, and these corresponding space-time theories. The subject of this thesis is to address these questions in certain cases. <p> <p> This dissertation is divided in three parts.<p> <p> In Part I, we first review the mathematical background on Kac-Moody algebras required to understand the results of this thesis. We then describe the investigations of the underlying symmetry structure of supergravity theories.<p> <p> In Part II, we focus on the bosonic sector of eleven-dimensional supergravity which would be invariant under the extended symmetry E_{11}. We study its subalgebra E_{10} and more precisely the real roots of its affine subalgebra E_9. For each positive real roots of E_9 we obtain a BPS solution of eleven-dimensional supergravity or of its exotic counterparts. All these solutions are related by U-dualities which are realized via E_9 Weyl transformations.<p> <p> In Part III, we study the symmetries of pure N=2 supergravity in D=4. As is known, the dimensional reduction of this model with one Killing vector is characterized by a non-linearly realized symmetry SU(2,1). We consider the BPS brane solutions of this theory preserving half of the supersymmetry and the action of SU(2,1) on them. Infinite-dimensional symmetries are also studied and we provide evidence that the theory exhibits an underlying algebraic structure described by the Lorentzian Kac-Mody group SU(2,1)^{+++}. This evidence arises from the correspondence between the bosonic space-time fields of N=2 supergravity in D=4 and a one-parameter sigma-model based on the hyperbolic group SU(2,1)^{++}. It also follows from the structure of BPS brane solutions which is neatly encoded in SU(2,1)^{+++}. As a worthy by-product of our analysis, we obtain a regular embedding of su(2,1)^{+++} in E_{11} based on brane physics./<p><p> Nombreuses sont les recherches récentes indiquant que différentes théories de gravité couplée à un certain type de champs de matière pourraient être caractérisées par des algèbres de Kac-Moody. Celles-ci généreraient des symétries infinies-dimensionnelles. L'existence possible de ces symétries a motivé la reformulation de ces théories par des actions explicitement invariantes sous les transformations du groupe de Kac-Moody. Ces actions sont construites en termes d'une infinité de champs associés à l'infinité de générateurs de l'algèbre correspondante. Si la conjecture de ces symétries est exacte, qu'en est-il de l'interprétation de l'infinité de champs? Qu'en est-il d'autre part de la correspondance entre ces actions explicitement invariantes sous les groupes de Kac-Moody et les théories d'espace-temps correspondantes? C'est autour de ces questions que gravite cette thèse.<p><p><p>Nous nous sommes d'abord focalisés sur le secteur bosonique de la supergravité à 11 dimensions qui possèderait selon diverses études une symétrie étendue E_{11}. Nous avons étudié la sous-algèbre E_{10} et plus particulièrement les racines réelles de sa sous-algèbre affine E_9. Pour chacune de ces racines, nous avons obtenu une solution BPS de la supergravité à 11 dimensions dépendant de deux dimensions d'espace non-compactes. Cette infinité de solutions résulte de transformations de Weyl successives sur des champs dont l'interprétation physique d'espace-temps était connue. <p><p>Nous avons ensuite analysé les symétries de la supergravité N=2 à 4 dimensions dont le secteur bosonique contient la gravité couplée à un champ de Maxwell. Cette théorie réduite sur un vecteur de Killing est caractérisée par la symétrie SU(2,1). Nous avons considéré les solutions de brane BPS qui préservent la moitié des supersymétries ainsi que l'action du groupe SU(2,1) sur ces solutions. Les symétries infinies-dimensionnelles ont également été étudiées. D'une part, la correspondance entre les champs d'espace-temps de la théorie N=2 et le modèle sigma basé sur le groupe hyperbolique SU(2,1)^{++} est établie. D'autre part, on montre que la structure des solutions de brane BPS est bien encodée dans SU(2,1)^{+++}. Ces considérations argumentent le fait que la supergravité N=2 possèderait une structure algébrique décrite par le groupe de Kac-Moody Lorentzien SU(2,1)^{+++}.<p> / Doctorat en Sciences / info:eu-repo/semantics/nonPublished

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This thesis is concerned with the Schrödinger representation of quantum field theory. We describe techniques for solving the Schrödinger equation which supplement the standard techniques of field theory. Our aim is to develop these to the point where they can readily be used to address problems of current interest. To this end, we study realistic models such as gauge theories coupled to dynamical fermions. For maximal generality we consider particles of all physical spins, in various dimensions, and eventually, curved spacetimes. We begin by considering Gaussian fields, and proceed to a detailed study of the Schwinger model, which is, amongst other things, a useful model for (3+1) dimensional gauge theory. One of the most important developments of recent years is a conjecture by Mal-dacena which relates supergravity and string/M-theory on anti-de-Sitter spacetimes to conformal field theories on their boundaries. This correspondence has a natural interpretation in the Schrödinger representation, so we solve the Schrödinger equation for fields of arbitrary spin in anti-de-Sitter spacetimes, and use this to investigate the conjectured correspondence. Our main result is to calculate the Weyl anomalies arising from supergravity fields, which, summed over the supermultiplets of type JIB supergravity compactified on AdS(_s) x S(^5) correctly matches the anomaly calculated in the conjecturally dual N = 4 SU{N) super-Yang-Mills theory. This is one of the few existing pieces of evidence for Maldacena's conjecture beyond leading order in TV.

Abstract The collective field theory technique provides a method of tackling problems with two N × N matrices in the large N limit. The collective field background from one matrix is first found, then the second matrix is introduced into this background as an impurity. Within the context of the AdS/CFT correspondence, this technique can be used to describe gauge theory states in the BMN limit. This dissertation starts by developing the collective field theory technique, firstly in general variables, then for one matrix, and subsequently for two matrices. It goes on to introduce a Yang-Mills interaction term, where two variable identifications are considered. The first is the more traditional angular momentum eigenstate model. The second is a model that directly uses two of the Higgs scalars. This model has been mentioned in the literature, but has not been considered in great depth. The exact two impurity spectrum is found, and the multi-impurity spectrum is found to first order. The resulting energy values match a spectrum that has been found for giant magnons.

O modelo não linear supersimétrico em l+l dimensões é acoplado à supergravidade. Ao quantizarmos a teoria, os campos de matéria adquirem massa dinamicamente, o que ocasiona a quebra da invariança de Weyl. Este fato implica em que as funções de dois pontos do Gravitino e do Graviton, obtidas a partir da ação efetiva, não sejam triviais. Em particular a função de dois pontos do Gravitino apresenta um polo no infravermelho. Nós conjeturamos que este polo está ligado com o confinamento dos graus de liberdade supersimétricos da teoria. Isto porque, ao restringirmos o domínio de integração de x IND. 1 à uma medida finita L (quebrando as invarianças da teoria), aparece na função de dois pontos do Gravitino um termo de massa, que decresce exponencialmente em função de L. Neste contexto relacionamos este model o como da corda supersimetrica e definimos um critério de estabilidade para a mesma. / The nonlinear o supersymmetric model in l+l dimensions is coupled to supergravity. When we quantize the theory, the matter fields acquire mass dynamically, which leads to the breaking of the Weyl invariance. This fact implies that the two point functions of the Gravitino and the Graviton, obtained from the effective action, become non trivial. Particularly, the two point function of the Gravitino presents a pole in the infrared region. We conjecture that this pole is related to the confinement of all supersymmetric degrees of freedom of the theory. If we restraind the integration domain of x1 to a finite lengh L (breaking all invariances of the theory), there appears a mass term in two point function of the Gravitino, which decreases exponentially with L. In this context we relate this model with that of the supersymmetric string and define a stability criteria for the latter.

O escopo deste mestrado é de se familiarizar com a chamada {\\it correspondência AdS/CFT}, que tem sido um dos mais importantes desenvolvimentos na física teórica nas últimas décadas. De acordo com essa correspondência, deformações das geometrias do lado da gravidade (ou lado \"AdS\") devem ser mapeadas para operadores das teorias de calibre duais (ou lado \"CFT\"). Em particular, nos temos estado interessados em explorar uma entrada particular no dicionário AdS/CFT, a relação entre os operadores 1/2 BPS em ${\\cal N}=4$ super Yang-Mills, e as chamadas {\\it geometrias bubbling} no lado da gravidade. A fim de fazer isso, apresentamos primeiramente as noções de ${\\cal N}=4$ SYM e soluções de Supergravidade. Portanto, podemos expor mais claramente o sentido da correspondência AdS /CFT, e depois mostrar a derivação das geometrias 1/2 BPS duais a estados 1/2 BPS em ${\\cal N}=4$ SYM como um exemplo. / The scope of this Master program was to get acquainted with the so-called {\\it AdS/CFT correspondence}, which has been one of the most important developments in theoretical physics in the last decades. According to this correspondence, deformations of the geometries in the gravity side (or \"AdS\" side) must be mapped to states of the dual gauge theories (or \"CFT\" side). In particular, we have been interested in exploring a particular entry in the AdS/CFT dictionary, namely, the relation between 1/2 BPS operators in ${\\cal N}=4$ super Yang-Mills, and the so-called {\\it bubbling geometries} on the gravity side. In order to do that, we first present the notions of N=4 SYM and Supergravity solutions. In this way, we can expose the statement of the AdS/CFT correspondence, and later show the derivation of 1/2 BPS geometries dual to 1/2 BPS states in N=4 SYM as an example of this one.

Motivated by the AdS/CFT correspondence, new supersymmetric solutions to Type IIB and Type IIA supergravity are presented. These solutions contain $AdS_5$ or $AdS_4$ factors and are generated using T-duality symmetries of supergravity. The technique used to generate these solutions consists of performing a series of non-Abelian and Abelian T-dualities, sometimes with coordinate shifts in-between, to Freund-Rubin type seed backgrounds. An added bonus of the gauge fixing procedure inherent in non-Abelian T-Duality is the freedom to generate backgrounds with extra free parameters, some examples of which are presented. Aspects of the dual field theories of these new solutions are analyzed using holography techniques. The supersymmetry of these new backgrounds is also discussed. In addition to supergravity backgrounds with AdS, the study of generalized Calabi-Yau manifolds in the context of flux compactifications is briefly reviewed. The particular case of the resolved cone over $Y^{p,q}$ and its admission of generalized SU(3) structure solutions is examined. Contrary to geometries with $AdS$ factors, whose field theory duals are conformal field theories, these types of geometries can be phenomenologically interesting to study, as their gauge theory duals are minimally supersymmetric and confining, thus they could someday help aid our understanding of strongly-coupled QCD (Quantum Chromodynamics).