In this thesis we study the Einstein-Aether (E-A) theory from the point of view of its cosmological perturbations. We are interested in the constraints that may be obtained from this analysis and the special features that can arise from the vector mode, absent in General Relativity. We apply the theory of linear perturbations in an expanding universe to describe the growth of inhomogeneities on subhorizon scales after recombination. We can split the perturbations in the different modes (scalar, vector and tensor) and we can study each of them separately. This allow us to obtain the stability conditions for this kind of theories and we can also obtain the power spectrum for each mode. For the scalar modes, we calculate the subhorizon solutions during the radiation and matter domination epochs. We are also interested in the effect of the theory in the Cosmic Microwave Background anisotropies, in particular in the contribution of the vector modes, as these modes are absent in General Relativity. We analyze the solutions for radiation and matter and calculate the angular power spectrum at large and small angular scales. This allows us to compare the contribution of the vector modes with the one coming from the tensor ones and with observations. The last issue we address is the effects of the vector modes in the polarization of the Cosmic Microwave Background. / L’objectiu d’aquesta tesi és estudiar la teoria d’Einstein-Aether des del punt de vista de les pertorbacions cosmològiques. Estem interessats en les restriccions pels paràmetres de la teoria que es poden obtenir d’aquesta anàlisi i en les característiques particulars que pot generar el mode vectorial, absent en Relativitat General. Podem fer servir la teoria de pertorbacions lineals en un univers en expansió per descriure el creixement de les inhomogeneïtats a escales subhoritzó després de recombinació. Separem les pertorbacions en els diferents modes escalar, vectorial i tensorial i estudiem cada un d’ells separadament. Això ens permetrà obtenir les condicions d'estabilitat d'aquestes teories així com l’espectre de potències per cada un d'aquests modes. En el cas de l’escalar, calculem les solucions de subhoritzó durant les èpoques de radiació i matèria També estem interessats en l'efecte de la teoria d’Einstein-Aether en les anisotropies del fons còsmic de microones, en particular en la contribució dels modes vectorials, inexistent pel cas de Relativitat General. Analitzem les solucions per a radiació i matèria i calculem l’espectre de potències angular tant a escales angulars petites com a escales angulars grans. Comparem els resultats amb la contribució procedent del mode tensorial i amb les observacions. L'última qüestió que abordem és l'efecte que el mode vectorial té en la polarització del fons còsmic de radiació.

The fuzzball model of a black hole is an attempt to resolve the many paradoxes and puzzles of black hole physics that have revealed themselves over the last century. These badly behaved solutions of general relativity have given physicists one of the few laboratories to test candidate quantum theories of gravity. Though little is known about exactly what lies beyond the event horizon, and what the ultimate fate of matter that falls in to a black hole is, we know a few intriguing and elegant semi-classical results that have kept physicists occupied. Among these are the known black hole entropy and the Hawking radiation process.

FundaÃÃo Cearense de Apoio ao Desenvolvimento Cientifico e TecnolÃgico / Nesse trabalho à analizado a localizaÃÃo de fÃrmions de spin 1/2 em um bulk D-dimensional em um cenÃrio de (D-2)-branas. O modelo usado para tal à uma extensÃo para mais dimesÃes dos modelos Randall-Sundrum (RS) e de brana espessa. Ele à conhecido como modelo de codimensÃo 1. Os resultados obtidos sÃo fundamentados em uma geometria nÃo-fatorizÃvel do tipo Anti-de Sitter. Durante o processo de localizaÃÃo do modo zero, usa-se tanto a mÃtrica de Randall-Sundrum como uma mÃtrica com fator de dobra suave que depende da coordenada da dimensÃo extra, frequentemente usada nos modelos de brana espessa. As representaÃÃes de spin 1/2 variam com a dimensÃo do espaÃo-tempo, entÃo o processo de localizaÃÃo deve levar em conta a dimensionalidade do bulk. Baseados nesses modelos, descobre-se que a localizaÃÃo de fÃrmions em (D-2)-branas muda quando o espaÃo-tempo à par ou Ãmpar. Eles nÃo sÃo localizados quando a dimensionalidadedo bulk à par e somente uma das quiralidades pode ser localizada quando D à Ãmpar. / In this work we analyzed the localization of fermions of spin-1/2 in a D-dimensional bulk in a (D-2)-branes scenario. The model used for this is a dimensional extension of models Randall-Sundrum (RS) and thick branes. It is known as co-dimension 1 model. The obtained results are based in no-factorizable geometry type Anti-de Sitter. During the zero mode localization process, it is uses both the Randall-Sundrum metric as a metric with smooth warped factor that depends on the coordinate of extra dimension, frequently used in thick brane models. As the spin-1/2 representations change with dimension of spacetime, the localization process, somehow, must take into account the dimensionality of bulk. Based on these models, one finds that the localization fermions in (D-2)-branes changes when the spacetime is par or odd. They are not located when the dimensionality of bulk is par an only one of chiralities can be located when D is odd.

Orientador: Patricio Anibal Letelier Sotomayor / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Fisica Gleb Wataghin / Made available in DSpace on 2018-08-10T14:48:16Z (GMT). No. of bitstreams: 1 DiazPolanco_JoseLuisBernardo_D.pdf: 1702870 bytes, checksum: b78c0c03a9b2631b73aa3127ce3e7c0b (MD5) Previous issue date: 2008 / Resumo: Apresentamos duas soluções analíticas das equações de Einstein: A primeira para o caso estático no qual um fluido carregado está em torno de um corpo massivo com propriedades magnétic~ do tipo dipolar. Esta solução se reduz à solução de Gutsunaev-Manko [Ts.I. Gutsunaev , V .8. Manko Phys. Lett. 5, 215, 19851 se o fluido carregado desaparece. Encontramos que o balanço entre os campos acoplados é devido à existência de fluxos de energia (térmica e eletromagnética) auto-compensados. A pressão de radiação compensa os efeitos dinâmicos do fluido ao redor do corpo central. Estudamos os fluxos de energia no sistema e suas propriedades termodinâmicas. Encontramos o estado termodinâmico do sistema. Esta solução contém a solução de 8chwarzschild como caso particular . A segunda solução descreve um dipolo magnético massivo e irradiante. Esta solução é dependente do tempo e descrevemos cada uma das grandezas que participam na solução. Analisamos os fluxos de energia do sistema e notamos que a radiação do dipolo diminui com o tempo chegando num estágio final do tipo dipolo magnético massivo no vácuo. Torna-se interessante pensar na possibilidade de observação destes fluxos de energia na vizinhança de objetos estrelares compactos com propriedades magnéticas extremas / Abstract: We derive analytical solutions of the Einsteinfs equations for two different cases: The first one, a static case, in which a charged fluid is around a mass with extreme magnetic properties of the dipole type. This solution reduces to the Gutsunaev-Manko solution [Ts.I. Gutsunaev , V .S. Manko Phys. Lett. 5, 215, 19851 in the abscense of the charged fluid. We found that the gravitational equilibrium of the system is achieved when the energy fluxs ( thermal and electromagnetic) are balanced and the effective radiation pressure compensates the gravitational effects in the fluid. We study the flows of energy in the system and their thermodynamics properties, we found an analytical expression for the thermodynamic state of the coupled systems. This solution contains the Schwarzschild solution as a particular case. The second solution describes a massive magnetic dipole emiting radiation decreasing in time. In this case we also found the thermodynamic state of the system. As a conclusion, we believe that our theoretical model can be applied to compact stellar systems with extreme magnetic properties / Doutorado / Relatividade e Gravitação / Doutor em Ciências

Orientador: Ricardo Antonio Mosna / Dissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Matemática, Estatística e Computação Científica / Made available in DSpace on 2018-08-16T04:10:22Z (GMT). No. of bitstreams: 1 Nascimento_DaniloBorimdo_M.pdf: 2195612 bytes, checksum: 9db76fa3dc3fca1c9128da411fe240b5 (MD5) Previous issue date: 2010 / Resumo: No espaço euclidiano, deformações de corpos quase-rígidos podem gerar rotações globais líquidas que obedecem, em cada instante, a lei de conservação do momento angular (o problema do gato caindo é um exemplo). Em espaços curvos, um ciclo de deformações de um corpo pode gerar não só rotações, mas também translações globais. Este fenômeno é conhecido como efeito swimming, ou natação. Avron e Kenneth apresentaram recentemente um modelo físico para descrever este fenômeno [Avron JE, Kenneth O, New J. Phys. 8, 68 (2006)]. Os autores tratam de corpos compostos por um conjunto de massas puntiformes em variedades estáticas (no contexto não-relativístico) e calculam o deslocamento obtido por um ciclo de deformações infinitesimais. Tal deslocamento é então relacionado, no caso de corpos pequenos, à curvatura do espaço ambiente. Nesta dissertação, propomos uma nova formulação para o efeito swimming utilizando formalismo de fibrados e conexões. O espaço de configurações do sistema é descrito como o espaço total de um fibrado principal, cujo espaço base é dado pelo espaço dos formatos do sistema e o grupo estrutural é (essencialmente) dado pelas isometrias da variedade ambiente. Dotando o fibrado de uma conexão que carrega consigo a informação sobre as leis físicas de conservação, expressamos o ciclo de deformações como uma curva fechada no espaço base, o movimento do corpo como o levantamento horizontal desta curva e o deslocamento resultante como a holonomia da mesma. Por meio deste formalismo, sistematizamos o cálculo do deslocamento gerado por ciclos de deformações arbitrárias, além de obter, em cada instante e analiticamente, a evolução temporal do sistema em questão / Abstract: In Euclidean space, cyclic deformations of quasi-rigid bodies can lead to net global rotations even though they satisfy, at each moment, the angular momentum conservation law (the falling cat problem is an example). In curved spaces, cyclic changes in the body shape can also lead to rotations, but also to global translations. This phenomenon is known as the swimming effect. In a recent work, Avron and Kenneth developed a formalism to describe this phenomenon in the non-relativistic context [Avron JE, Kenneth O, New J. Phys. 8, 68 (2006)], which may be used to calculate the net displacement caused by an infinitesimal cycle of deformations of a given body. This displacement is then related, for small swimmers, to the curvature of the ambient space. In the present work, we propose a new formulation for the swimming effect in terms of principal bundles and connections. The configuration space of the system is described by the total space of a principal bundle, whose base space is given by the space of shapes of the body and whose structural group is (essentially) given by the isometries of the ambient manifold. A given deformation cycleof the body then corresponds to a loop in the base space. By defining a connection in this bundle which conveys the physical conservation laws of the system, the corresponding physical motion of the body is then given by the horizontal lift of this curve in the base space, while the net displacement of the body is given by the holonomy associated with this loop. As a result we obtain, in a systematical way, the displacement generated by arbitrary deformation cycles and we get, for each instant of time, the time evolution of the system analytically / Mestrado / Geometria e Topologia / Mestre em Matemática

Estudamos as restrições impostas pelo princípio da covariância sobre o procedimento de quantização em espaços planos e curvos. Mostramos que o conjunto de todas as quantizações covariantes em espaços planos em coordenadas retangulares é composto de ordenamentos de operadores de posição e momento e exibimos uma parametrização funcional deste conjunto. Deduzimos regras para a quantização covariante em espaços planos em coordenadas gerais. Generalizamos estas quantizações para espaços curvos e mostramos que nestes espaços, além da ambiguidade de ordenamento, surge uma nova ambiguidade relacionada à curvatura. Este novo tipo de ambiguidade explica o surgimento de uma classe grande de potenciais quânticos no problema da quantização de uma partícula não relativística em um espaço curvo. / We study the restrictions imposed by the covariance principle on the quantization procedure in flat and curved spaces. We show that the set of all covariant quantizations in flat spaces in rectangular coordinates is composed of position and momentum operator orderings and exhibit a functional parametrization of this set. We deduce rules for the covariant quantization in flat spaces in general coordinates. We generalize these quantizations for curved spaces and show that in such spaces, besides the ordering ambiguity, it appears a new ambiguity related to the curvature. This new kind of ambiguity explains the appearence of a wide class of quantum potentials in the problem of quantization of a non-relativistic particle in curved space.

Abstract not available

[Truncated abstract] As gravitational wave detectors approach sensitivities that will allow observations to become routine, astrophysics lies on the cusp of an exciting new era. Potential sources will include transients such as merging neutron stars and black holes, supernova explosions or the engines that power gamma-ray bursts. This thesis will be devoted to the astrophysical gravitational wave background signal produced by cosmological populations of such transient signals. Particular attention will be devoted to the observation-time dependence imposed on the individual sources that accumulate to produce a gravitational wave background signal. The ultimate aim is to determine what information is encoded in the temporal evolution of such a signal. To lay the foundations for further investigation, the stochastic gravitational wave background signal from neutron star birth throughout the Universe has been calculated. In view of the uncertainties in both the single-source emissions and source rate histories, several models of each are employed. The results show that that the resulting signals are only weakly dependent on the source-rate evolution model and that prominent features in the single-source spectra can be related to the background spectra. In comparison with previous studies, the use of relativistic single-source gravitational wave waveforms rather than Newtonian models and a more slowly evolving source-rate density results in a 1 { 2 order of magnitude reduction in signal. ... A comparison with the more commonly used brightness distribution of events shows that when applying both methods to a data stream containing a background of Gaussian distributed false alarms, the brightness distribution yielded lower standard errors, but was biased by the false alarms. In comparison, a fitting procedure based on the time evolution of events was less prone to errors resulting from false alarms, but as fewer events contributed to the data, had a lower resolution. In further support of the time dependent signature of transient events, an alternative technique is fiapplied to the same source population. In this case, the local rate density is probed by measuring the statistical compatibility of the filtered data against synthetic time dependent data. Although this method is not as compact as the fitting procedure, the rate estimates are compatible. To further investigate how the observation time dependence of transient populations can be used to constrain global parameters, the method is applied to Swift long gamma-ray burst data. By considering a distribution in peak °ux rather than a gravitational wave amplitude, gamma-ray bursts can be considered as a surrogate for resolved gravitational wave transients. For this application a peak °ux{observation time relation is described that takes the form of a power law that is invariant to the luminosity distribution of the sources. Additionally, the method is enhanced by invoking time reversal invariance and the temporal cosmological principle. Results are presented to show that the peak °ux{observation time relation is in good agreement with recent estimates of source parameters. Additionally, to show that the intrinsic time dependence allows the method to be used as a predictive tool, projections are made to determine the upper limits in peak °ux of future gamma-ray burst detections for Swift.

The fuzzball model of a black hole is an attempt to resolve the many paradoxes and puzzles of black hole physics that have revealed themselves over the last century. These badly behaved solutions of general relativity have given physicists one of the few laboratories to test candidate quantum theories of gravity. Though little is known about exactly what lies beyond the event horizon, and what the ultimate fate of matter that falls in to a black hole is, we know a few intriguing and elegant semi-classical results that have kept physicists occupied. Among these are the known black hole entropy and the Hawking radiation process.

Orientador: Patricio Anibal Letelier Sotomayor / Dissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Matematica, Estatistica e Computação Cientifica / Made available in DSpace on 2018-08-10T23:13:00Z (GMT). No. of bitstreams: 1 Manoel_JoaoPauloPitelli_M.pdf: 2107794 bytes, checksum: 5fe60d22c5d7bd4e165a24c4c9c6d375 (MD5) Previous issue date: 2008 / Resumo: Espaços-tempos classicamente singulares são estudados utilizando-se partículas quânticas (ao invés de clássicas) obedecendo as equações de Klein-Gordon e Dirac, a fim de determinar se estes espaços permanecem singulares do ponto de vista quântico. Primeiramente é apresentada uma revisão do ferramental matemático necessário para o estudo de singularidades quânticas, cujo principal resultado utilizado é a teoria de índices deficientes devido a von Neumann. No apêndice A é apresentado um primeiro estudo sobre singularidades quânticas em espaços-tempos com defeitos topológicos numa superfície 2-dimensional (paredes cósmicas), em especial superfícies esféricas e cilíndricas. Estes espaços continuam singulares nesta teoria e todas as informações extras (que em mecânica quântica se apresentam sob a forma de condições de contorno) necessárias para se remover a singularidade são encontradas. No apêndice B, é estudado um espaço-tempo 2+1 dimensional com curvatura negativa constante. É mostrado que este espaço permanece singular quando visto pela mecânica quântica e as condições de contorno possíveis são encontradas utilizando-se resultados obtidos no caso plano / Abstract: Classical singular spacetimes are studied using quantum particles (instead of classical ones) obeying Klein-Gordon and Dirac equations, to determine if these spacetimes remain singular in the view of quantum mechanics. First we give a review of the mathematical framework necessary to study quantum singularities, wich the main result to be used later is von Neumann¿s theory of deficient indices. In appendix A, a first work on quantum singularities in spacetimes with topological defects on a 2-dimensional hypersurface (cosmic walls), specifically spherical and cylindrical surfaces, is presented. These spacetimes remain singular in this theory and all extra informations (which in quantum mechanics correspond to boundary conditions) necessary to remove the naked singularity are found. In Apendix B, a 2+1 dimensional spacetime with constant negative curvature is studied. It is shown that this spacetime remains quantum mechanically singular and all possible boundary conditions are found using results obtained in plane case / Mestrado / Relatividade Geral/Gravitação Quantica / Mestre em Matemática Aplicada