In this thesis we review and build on the common methods used to analyze null geodesics in Schwarzschild de Sitter space. We present a general technique which allows finding measurable intersection angles of null trajectories analytically, and as one of its applications we establish a general relativistic aberration relationship. The tools presented are used to analyze some standard setups of gravitational deflection of light and gain a clear understanding of the role that the cosmological constant, Λ, plays in gravitational lensing phenomena. Through reviewing some recent papers on the topic with the present results in mind, we attempt to explain the major sources of disagreement in the ongoing debate on the subject, which started with Rindler and Ishak’s original paper, regarding the influence of Λ on lensing phenomena. To avoid ambiguities and room for misunderstanding we present clear definitions of the quantities used in the present analysis as well as in other papers we discuss. / Thesis (Master, Physics, Engineering Physics and Astronomy) -- Queen's University, 2013-09-30 21:18:26.762

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In this thesis we present work done in an analysis of models of brane induced gravity. These are higher dimensional generalizations of Einstein's General relativity where our universe is considered as a brane in a higher dimensional bulk and where the gravitational dynamics on the brane is enhanced. This provides a modification of gravity on the brane as compared to ordinary general relativity, primarily at very large distances. These models are therefore very interesting for adressing the cosmological constant problem. Even though the basic setup is natural to consider from the perspective of effective field theory and also follow from certain string theoretical considerations, the models have been plagued by inconsistencies in the form of unstable modes. In particular, a ghostlike and tachyonic scalar mode appears already at the linear level in a perturbative treatment. In order to gain a deeper insight into the nature of these consistency problems we have revisited the models, performing a more extensive analysis of the generic models than has previously been done. We have worked entirely in a gauge invariant formalism in order not to be obscured by gauge issues. We have also incorporated an effective thickness of the brane in our analysis and performed an explicit analysis of the effect of contributions from the extrinsic geometry. Although our analysis has been carried out at the linear level in a perturbative treatment we are able to get a deeper understanding of the unstable mode and illuminate some of the difficulties of these models that would likely persist even in a full nonlinear analysis.

Submitted by Vasti Diniz (vastijpa@hotmail.com) on 2017-09-13T13:50:59Z No. of bitstreams: 1 arquivototal.pdf: 2320909 bytes, checksum: 25cc6b6504385f6f69412717c2952be1 (MD5) / Made available in DSpace on 2017-09-13T13:50:59Z (GMT). No. of bitstreams: 1 arquivototal.pdf: 2320909 bytes, checksum: 25cc6b6504385f6f69412717c2952be1 (MD5) Previous issue date: 2016-07-29 / We considered the discrete approach to Newtonian cosmology presented by Ellis and Gibbons in a recent paper, and generalize this to the continuum limit. The results are obtained using the Newton's laws for particles interacting gravitationally, which are moving homothetically, with with their comoving positions constituting a central configuration. It requines no use of the fluid mechanics, but just a correspondence between the quantities which appear in the approach of Ellis and Gibbons and their generalizations for a system with high density, but with a finite number of particles. The solutions of the equation for the scale factor are presented, taking into account the presence of a term associated with the cosmological cons­tant. We briefly present the relativistic cosmology and compare with Newtonian cosmology. / Consideramos a formulagao discreta da cosmologia Newtoniana adotada por Ellis e Gibbons, em artigo recente, e fazemos uma generalizagao para o limite do continuo. Os resultados sao obtidos com o use das leis de Newton para particulas que interagem gravitacionalmente, que se movem homoteticamente, com suas coordenadas comOveis constituindo-se uma con­figuragao central. Nao foi necessario o use da mecanica dos fluidos, mas tao somente, uma correspondencia direta entre as grandezas discretas da formulagao de Ellis e Gibbons e suas generalizagoes para um sistema muito denso, com um nilmero finito de particulas. Sao apresentadas solugoes da equagao para o fator de escala, considerando a presenga do termo associado a constante cosmolOgica. E feita uma breve apresentagao da cosmologia Einstei­niana e uma comparagao com a cosmologia Newtoniana.

京都大学 / 新制・課程博士 / 博士(理学) / 甲第24869号 / 理博第4979号 / 新制||理||1711(附属図書館) / 京都大学大学院理学研究科物理学・宇宙物理学専攻 / (主査)教授 向山 信治, 准教授 樽家 篤史, 教授 橋本 幸士 / 学位規則第4条第1項該当 / Doctor of Science / Kyoto University / DFAM

Master of Science / Department of Physics / Bharat Ratra / In this report, we discuss the four standard energy conditions of General Relativity (null, weak, dominant, and strong) and investigate their cosmological consequences. We note that these energy conditions can be compatible with cosmic acceleration provided that a repulsive cosmological constant exists and the acceleration stays within certain bounds. Scalar fields and dark energy, and their relationships to the energy conditions, are also discussed. Special attention is paid to the 1988 Ratra-Peebles scalar field model, which is notable in that it provides a physical self-consistent framework for the phenomenology of dark energy. Appendix B, which is part of joint-research with Anatoly Pavlov, Khaled Saaidi, and Bharat Ratra, reports on the existence of the Ratra-Peebles scalar field tracker solution in a curvature-dominated universe, and discusses the problem of investigating the evolution of long-wavelength inhomogeneities in this solution while taking into account the gravitational back-reaction (in the linear perturbative approximation).

In this thesis, Newman-Penrose techniques are used to obtain some new exact solutions to Einstein's field equations of general relativity and to assist in the physical interpretation of some exact radiative space-times. Attention is restricted to algebraically special space-times with a twist-free, repeated principal null congruence. In particular, the Robinson-Trautman type N solutions, which describe expanding gravitational waves, are investigated for all possible values of the cosmological constant A and the Gaussian curvature parameter E. The wave surfaces are always (hemi-)spherical, with successive surfaces displaced along time-like, space-like or null lines, depending on E. Explicit sandwich waves of this class are studied in Minkowski, de Sitter or anti-de Sitter backgrounds and a particular family of such solutions, which can be used to represent snapping or decaying cosmic strings, is considered in detail. The singularity and global structure of the solutions is also presented. In the remaining part of the thesis, the complete family of space-times with a non-expanding, shear-free, twist-free, geodesic principal null congruence (Kundt waves), that are of algebraic type III and for which the cosmological constant (Ac) is non-zero, is presented. The possible presence of an aligned pure radiation field is also assumed. These space-times generalise the known vacuum solutions of type N with arbitrary Ac and type III with Ac = O. It is shown that there are two, one and three distinct classes of solutions when Ac is respectively zero, positive and negative and, in these cases, the wave surfaces are plane, spherical or hyperboloidal in Minkowski, de Sitter or anti-de Sitter backgrounds respectively. The singularities which occur in these space-times are interpreted in terms of envelopes of these wave surfaces. Again, by considering functions of the retarded time which "cross-over" between canonical types, sandwich waves are also studied. The limiting cases of these, giving rise to shock or impulsive waves, are also considered.

Submitted by Renata Lopes (renatasil82@gmail.com) on 2017-04-26T18:18:25Z No. of bitstreams: 1 monalisasilvadeoliveira.pdf: 473060 bytes, checksum: 1e394ef35b65c023c130f0dbca9a9d12 (MD5) / Approved for entry into archive by Adriana Oliveira (adriana.oliveira@ufjf.edu.br) on 2017-05-13T12:04:23Z (GMT) No. of bitstreams: 1 monalisasilvadeoliveira.pdf: 473060 bytes, checksum: 1e394ef35b65c023c130f0dbca9a9d12 (MD5) / Made available in DSpace on 2017-05-13T12:04:23Z (GMT). No. of bitstreams: 1 monalisasilvadeoliveira.pdf: 473060 bytes, checksum: 1e394ef35b65c023c130f0dbca9a9d12 (MD5) Previous issue date: 2013-02-28 / CAPES - Coordenação de Aperfeiçoamento de Pessoal de Nível Superior / Neste trabalho, fazemos uma pequena revisão sobre tensores e sua utilização na Relatividade Geral, apresentamos o método de transformação conforme e o teorema da fatorização e discutimos as soluções de Schwarzschild com e sem constante cosmológica. Então, a solução de Schwarzschild com constante cosmológica é derivada, a partir das equações de campo de Einstein, utilizando-se os conceitos abordados. / In this work, we make a brief review of tensors and their use in General Relativity, we present the local conformal transformation method and the factorization theorem and we discuss Schwarzschild's solutions with and without cosmological constant. Then, the Schwarzschild's solution with cosmological constant is derived, from the Einstein's field equations, using the concepts addressed.

In this work we investigate an exact solution of Einstein's equations which is described by the Pleba'nski-Demia'nski metric. This metric represents type D space-times and contains seven free parameters, including electric and magnetic charges and a cosmological constant. We study geometrical and phy- sical properties of these space-times in the case when repeated principal null congruences have zero expansion. Therefore, first we study de Sitter universe and anti-de Sitter universe in the Pleba'nski-Demia'nski coordinates, and we care- fully analyze the corresponding parametrizations of (anti-)de Sitter hyperboloid in five-dimensional flat space-time, unknown so far, we draw the respective con- formal diagrams, and we find transformations to various known forms. After that, we investigate the more general case of the B metrics with a cosmological con- stant, and we do a basic analysis of its geometrical properties. We summarize the article by Gott from 1974, where he interprets the BI metric as a part of space-time with a tachyon singularity, and we generalize his results for the case of non-zero cosmological constant. Finally, we analyze even more general cases of the Pleba'nski-Demia'nski metric with more non-zero parameters. In particular, we study the electromagnetic field in the case of non-zero...

As observações astronômicas dos últimos 15 anos revelaram que o universo atualmente está expandindo aceleradamente. No contexto da relatividade geral se acredita que a energia escura, cujo melhor candidato é a densidade do vácuo ($\\Lambda/8\\pi G$), é o agente responsável por este estado acelerado. No entanto, o termo $\\Lambda$ tem duas sérias dificuldades: o problema da constante cosmológica e o problema da coincidência. Com o objetivo de aliviar o problema da constante cosmológica, muitos modelos adotam um termo $\\Lambda$ dinâmico, permitindo seu decrescimento ao longo de toda a história cósmica. Neste tipo de modelo, a equação de conservação do tensor momento energia total exige uma troca de energia entre a densidade do vácuo e as outras componentes energéticas do universo; o que também alivia o problema da coincidência. Neste trabalho discutimos diferentes consequências de um vácuo dinâmico no âmbito cosmológico e no processo de colapso gravitacional. Em particular, analisamos o caso em que a densidade do vácuo possui uma dinâmica não trivial com a escala de energia típica do universo, que depende monotonamente do parâmetro de Hubble, decrescendo ao longo de toda a história cósmica. Nos referiremos a este modelo como modelo deflacionário. Nesse contexto, utilizando os primeiros termos da expansão para a densidade do vácuo, sugerida pela teoria do grupo de renormalização em espaço-tempos curvos, propomos um novo cenário cosmológico baseado numa densidade do vácuo dinâmica. O cenário proposto é completo no sentido de que o mesmo vácuo é responsável pelas duas fases aceleradas do universo, conectadas por uma fase de radiação e um estágio de domínio da matéria. Neste cenário o universo plano é não singular, iniciando sua evolução a partir de um estágio do tipo de Sitter e, portanto, toda a história cósmica ocorre entre duas fases de Sitter limites. Este modelo não apresenta o problema de horizonte, e nele a nucleossíntese cosmológica ocorre como no modelo de Friedmann, e embora este modelo seja muito próximo do modelo $\\Lambda$CDM, o grande acúmulo de observações no estágio recente do universo permitirão que este poda ser testado. Adicionalmente, mostraremos que generalizações do modelo deflacionário incluindo curvatura espacial apresentam propriedades e vantagens similares. Usando observações de $H(z)$, da luminosidade de supernovas tipo Ia, da função de crescimento linear das perturbações escalares, e da posição do pico das oscilações acústicas de bárions conseguimos vincular um dos parâmetros do modelo. Por outro lado, analisando a física do universo primordial, assumindo um vácuo não perturbado, conseguimos limitar um segundo parâmetro fazendo uso do índice espectral das perturbações escalares. Com o objetivo de fazer uma análise mais completa do modelo no âmbito cosmológico, analisamos também as possíveis restrições oriundas da validade da segunda lei da termodinâmica em sua forma generalizada (GSLT). Para isto investigamos a evolução tanto da entropia associada ao horizonte aparente do universo, que é um horizonte atrapante devido a que o escalar de Ricci é positivo, como do seu conteúdo material. Motivados pela forma como a singularidade primordial do universo é evitada devido aos efeitos do decaimento do vácuo, incluímos no presente trabalho outra linha de desenvolvimento: a análise dos estágios finais do processo de colapso gravitacional em presença de uma densidade do vácuo dinâmica. Centraremos esta análise na determinação de modelos que possam ou não evitar a formação de um buraco negro. Mostraremos que modelos com um termo de vácuo proporcional à densidade de energia total do sistema, não podem evitar a formação de uma singularidade no estágio final do processo de colapso. Adicionalmente obteremos correções para a massa colapsada, para o tempo de formação do horizonte e para o tempo de colapso como função dos parâmetros do modelo e da curvatura espacial. Por último analisaremos a influência de uma densidade do vácuo capaz de dominar sobre as outras componentes no regime de altas energias, mostrando que este tipo de dinâmica na densidade do vácuo evita a formação de um estado final singular. / The astronomical observations of the last 15 years revealed that the universe is currently undergoing an expanding accelerating phase. In the general relativity context is believed that dark energy, whose best candidate is the vacuum energy density $ho_v \\equiv \\Lambda/8\\pi G$, is the fuel responsible for the present accelerating stage. However, the so-called $\\Lambda$-term has two serious drawnbacks, namely: the cosmological constant problem and the coincidence problem. In order to alleviate the cosmological constant problem, many models adopt a dynamical $\\Lambda$ term, thereby allowing its decreasing throughout the cosmic history. In this kind of model, the total energy conservation law defined in terms of the energy momentum tensor requires an energy exchange between the vacuum and the material components of the universe, which also contributes to alleviate the coincidence problem. In the present thesis we discuss different consequences of an interacting vacuum component both in the cosmological scenario as well as in the process of gravitational collapse. In particular, in the cosmological domain, we examine the case where the vacuum has a nontrivial dynamics dependent on a typical energy scale, the Hubble parameter, that decreases in the course of the cosmic history. We will refer to this model as deflationary model. In this context, by using a truncated expansion for the vacuum energy density, as suggested by the renormalization group theory in curved space-time, we propose a new cosmological scenario based on a dynamical $\\Lambda$-term. The proposed scenario is complete in the sense that the same vacuum is responsible for both accelerating phases of the universe, which are linked by two subsequent periods of radiation and non-relativistic matter domination. In this scenario the flat universe is nonsingular and starts its evolution from an asymptotic de Sitter stage, so that the cosmic story takes place between two extreme de Sitter phases. The model is free of the horizon problem as well as of the \"graceful exit\" problem plaguing many inflationary variants. In addition, the cosmological nucleosynthesis occurs as in the Friedmann model and the observations in the latest stages of the universe can potentially differentiate between the deflationary and the standard $\\Lambda$CDM model. The generalizations including spatial curvature are aslo discussed in detail. On the other hand, by using the late time tests like type Ia supernovae, the redshift dependence of the Hubble parameter, $H(z)$, the linear growth function of scalar perturbations, and the peak position of baryon acoustic oscillations we have constrained the basic parameters of the model. Conversely, analyzing the physics of the primordial universe and assuming that the vacuum is a smooth component, we have also constrained the spectral index of scalar density perturbations. In order to establish a more complete analysis of our cosmological scenario, we also discuss the possible constraints arising from the validity of the generalized second law of thermodynamics, that is, by including the horizon thermodynamics. Since the apparent horizon of the universe behaves like a trapped horizon because the Ricci scalar is positive, we investigate the evolution of both the entropy of the material components and the entropy associated to the horizon. Motivated by the avoidance of the Big-Bang singularity due to the decaying vacuum effects, we have explored another line of development: the analysis of the final stages of gravitational collapse process in the presence of a dynamic vacuum. This analysis focused on the determination of models able to prevent or not the formation of a black hole. In this connection, we shown that the presence of an interacting vacuum proportional to the total energy density of the system does not prevent the formation of a singularity in the final stages of the collapsing process. In addition, we obtain corrections for the collapsed mass, the horizon time formation and the collapsing time as a function of the free parameters and the spatial curvature of the models. Finally, we have also analyzed the influence of a vacuum contribution which dominates the other components into the high energy limit (due to the presence of higher orders terms in the contraction rate), and shown that for this kind of models the growth of the vacuum energy density prevents the formation of the singularity.