Les prédictions d'inflation du spectre de puissance de la perturbation de la courbure ont déjà fait l’objet de vérification d’un excellent niveau, permettant à de nombreux modèles de rester compatibles avec les observations. Dans la présente thèse, nous avons étudié les corrélations de troisième ordre qui pourraient permettre de mieux distinguer les différents modèles d'inflation les uns des autres. Parmi toutes les extensions possibles du modèle standard d'inflation, nous avons choisi d'étudier des modèles de deux champs scalaires à termes cinétiques standards et à métrique des champs plat. La nouveauté introduite par ces modèles est la présence de la perturbation d'isocourbure. Son interaction avec la perturbation adiabatique hors de l'horizon produit des non-linéarités caractéristiques des modèles à plusieurs champs scalaires. Dans, ce contexte, nous avons établi la forme de la perturbation adiabatique et de la perturbation d'isocourbure invariant sous transformations de jauge en deuxième ordre. De plus, nous avons trouvé l'action de troisième ordre qui décrit leurs interactions. En outre, nous avons élaboré le formalisme des grandes longueurs d'onde afin d'obtenir une expression pour le paramètre de non-gaussiannité fNL en fonction du potentiel des champs. Nous avons ensuite, utilisé cette formule pour traiter analytiquement - avec l'hypothèse de slow-roll - des classes générales de potentiels et vérifier nos résultats numériquement par la théorie exacte. De là, nous avons pu tirer des conclusions générales concernant les propriétés de fNL, comme par exemple la dépendance de sa magnitude des caractéristiques du trajet des champs et de la perturbation d'isocourbure, ainsi que sa dépendance de la magnitude et de la taille relative des trois impulsions dont le corrélateur à trois points est fonction. / Inflationary predictions for the power spectrum of the curvature perturbation have been verified to an excellent degree, leaving many models compatible with observations. In this thesis we studied third-order correlations, that might allow one to further distinguish between inflationary models. From all the possible extensions of the standard inflationary model, we chose to study two-field models with canonical kinetic terms and flat field space. The new feature is the presence of the so-called isocurvature perturbation. Its interplay with the adiabatic perturbation outside the horizon gives birth to non-linearities characteristic of multiple-field models. In this context, we established the second-order gauge-invariant form of the adiabatic and isocurvature perturbation and found the third-order action that describes their interactions. Furthermore, we built on and elaborated the long-wavelength formalism in order to acquire an expression for the parameter of non-Gaussianity fNL as a function of the potential of the fields. We next used this formula to study analytically, within the slow-roll hypothesis, general classes of potentials and verified our results numerically for the exact theory. From this study, we deduced general conclusions about the properties of fNL, its magnitude depending on the characteristics of the field trajectory and the isocurvature component, as well as its dependence on the magnitude and relative size of the three momenta of which the three-point correlator is a function.

Inflationary predictions for the power spectrum of the curvature perturbation have been verified to an excellent degree, leaving many models compatible with observations. In this thesis we studied third-order correlations, that might allow one to further distinguish between inflationary models. From all the possible extensions of the standard inflationary model, we chose to study two-field models with canonical kinetic terms and flat field space. The new feature is the presence of the so-called isocurvature perturbation. Its interplay with the adiabatic perturbation outside the horizon gives birth to non-linearities characteristic of multiple-field models. In this context, we established the second-order gauge-invariant form of the adiabatic and isocurvature perturbation and found the third-order action that describes their interactions. Furthermore, we built on and elaborated the long-wavelength formalism in order to acquire an expression for the parameter of non-Gaussianity fNL as a function of the potential of the fields. We next used this formula to study analytically, within the slow-roll hypothesis, general classes of potentials and verified our results numerically for the exact theory. From this study, we deduced general conclusions about the properties of fNL, its magnitude depending on the characteristics of the field trajectory and the isocurvature component, as well as its dependence on the magnitude and relative size of the three momenta of which the three-point correlator is a function.

No description available.

Orientadores: Alex Eduardo de Bernardini, Marcelo Moraes Guzzo / Dissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Física Gleb Wataglin / Made available in DSpace on 2018-08-17T16:24:26Z (GMT). No. of bitstreams: 1 DuartePerico_EderLeonardo_M.pdf: 2896271 bytes, checksum: 3596fcdea9450fe936e36e96d5ffbad3 (MD5) Previous issue date: 2011 / Resumo: O assunto deste estudo é formação de estruturas em grandes escalas em um universo plano dominado por radiação, matéria escura fria e constante cosmológica como modelo de energia escura no caso particular de presença de um gás degenerado de férmions (GDF) não interagentes como fluído de teste. Nosso modelo admite uma evolução linear das perturbações cosmológicas como também se limita a perturbações escalares, responsáveis pela formação de estruturas. O objetivo principal é analisar a contribuição do GDF no espectro de potências da matéria no presente após uma evolução isentrópica das perturbações primordiais, e compará-la com resultados obtidos para neutrinos cosmológicos. Neste caso, teremos uma mudança contínua de comportamento do GDF de gás ultra-relativístico para não relativístico, o qual aconteceria durante o período de domínio da matéria. Com o objetivo de obter expressões analíticas para a evolução temporal das perturbações do GDF tivemos que fazer o estudo destas em quatro casos diferentes: no período de domínio da radiação, no período de domínio da matéria escura, na escala de super-horizonte durante a transição entre estes dois períodos, e finalmente no período de domínio da constante cosmológica. Fomos bem sucedidos ao chegar a resultados consistentes utilizando dois caminhos diferentes: no primeiro, usando a equação de conservação do tensor momento energia para um gás ideal de férmions totalmente degenerado e não interagente, e no segundo, usando a equação de Boltzmann para um gás de férmions fortemente degenerado e também não interagente. Os dois métodos analíticos levam à mesma solução para as perturbações do GDF quanto escritas até primeira ordem em teoria de perturbações. De forma complementar, os nossos resultados numérico mostram um aumento no espectro de potências da matéria para escalas intermediárias se comparado com a contribuição dos neutrinos massivos. Finalmente estendemos nossa análise numérica ao substituirmos a matéria escura fria CDM e a constante cosmológica por um gás generalizado de Chaplygin GCG como modelo efetivo para o setor escuro do universo, mantendo as condições de contorno que envolvem as densidades médias, e as condições iniciais para as perturbações / Abstract: The subject of this study is the formation of large scale structures (LSS) in a at universe dominated by radiation, cold dark matter and cosmological constant - as a dark energy model - in presence of a degenerate fermionic gas (GDF) as non-interacting test fluid. Our model assumes a linear evolution of cosmological perturbations as well as merely scalar perturbations responsible for structure formation. Our main objective is to analyze the contribution of the GDF in the matter power spectrum today, after an isentropic evolution of primordial perturbations and a continuous change of behavior of ultra-relativistic for non-relativistic GDF, which occurs during the matter domination era in our model. To obtaining analytical expressions for temporal evolution of the GDF perturbations we did study them in four different cases: during the radiation domination era, the dark matter domination, the super-horizon scale limit during the transition between these first two periods and finally during the cosmological constant domination era. We get these results using two different approaches: first, using the conservation equation of the stress-energy tensor for a perfect and non-interacting and fully degenerated fermionic gas, and second, using the Boltzmann equation for a non-interacting and strongly degenerated fermionic gas. Both methods lead to the same analytical solution for GDF perturbations at first order on perturbation theory. On the other hand, our numerical results show an increase in the power spectrum of matter for intermediate scales if compared it with the contribution of massive neutrinos. Finally, we show the change on the results of the standard model of cosmology (CDM) when we exchanging the cold dark matter CDM and the cosmological constant for a generalized Chaplygin gas GCG how effective model of twice old fluids with the same mean density of energy / Mestrado / Cosmologia / Mestre em Física

Submitted by isabela.moljf@hotmail.com (isabela.moljf@hotmail.com) on 2016-08-12T14:56:03Z No. of bitstreams: 1 thiagomorallesdeabreu.pdf: 433339 bytes, checksum: dc2019985b911c7c131a86a07cac34de (MD5) / Approved for entry into archive by Adriana Oliveira (adriana.oliveira@ufjf.edu.br) on 2016-08-15T13:36:51Z (GMT) No. of bitstreams: 1 thiagomorallesdeabreu.pdf: 433339 bytes, checksum: dc2019985b911c7c131a86a07cac34de (MD5) / Made available in DSpace on 2016-08-15T13:36:51Z (GMT). No. of bitstreams: 1 thiagomorallesdeabreu.pdf: 433339 bytes, checksum: dc2019985b911c7c131a86a07cac34de (MD5) Previous issue date: 2016-06-24 / CAPES - Coordenação de Aperfeiçoamento de Pessoal de Nível Superior / Na presente dissertação é apresentada uma revisão detalhada de modelos cosmológicos, incluindo a dinâmica de perturbações cosmológicas lineares para dois modelos que desempenham interesse do ponto de vista de possíveis aplicações. Todo material discutido é oriundo da literatura recente e não se apresenta elementos originais. Entretanto, o conhecimento desses modelos abre uma possibilidade de extensões que estão agora sob discussão e desenvolvimento. De início é feita uma sucinta exposição do Modelo Cosmológico Padrão, que pode ser associado com o modelo FLRW (Friedmann-Lemaître-Robertson-Walker). Este último descreve um Universo em expansão marcado pela homogeneidade e isotropia em grande escala. Após isso discute-se o modelo com fluido cósmico composto por gás relativístico reduzido, mais conhecido pela sigla RRG, do inglês "reduced relativistic gas". A equação de estado do modelo RRG tem uma correspondência bem próxima ao modelo de gás de partículas massivas com energias cinéticas relativísticas. Considera-se ainda as perturbações cosmológicas em torno do modelo RRG de fundo plano, homogêneo e isotrópico. Por fim, segue-se a discussão sobre a possibilidade de incluir perturbações na constante gravitacional G e na constante cosmológica Λ, no ramo do modelo motivado por correções semiclássicas. / In this thesis we present a detailed review of some cosmological models, including the theory of linear cosmological perturbations for two distinct models which represent certain interest from the point of view of possible applications. All presented material comes from the recent literature and does not include original elements. However, the knowledge of these models opens a possibility of extensions which are now under discussion and development. At first it is presented a brief review of the Standard Cosmological Model, which can be associated with FLRW model (Friedmann-Lemaître-Robertson-Walker). The latter describes an expanding Universe marked by homogeneity and isotropy on a large scale. After that we discuss the model composite by a cosmic fluid described by reduced relativisticgas,betterknownbytheacronymRRG(reducedrelativisticgas). Theequation of state of the RRG model has a very close match to the model of gas of massive particles with relativistic kinetic energies. We consider the cosmological perturbations around the background of flat, homogeneous and isotropic RRG-based model. After that follows the discussion of the possibility of including perturbations of the gravitational constant G and the cosmological constant Λ within the model motivated by semiclassical corrections.

L'un des plus grands problèmes ouverts de la cosmologie moderne est l'origine de l'expansion accélérée de l'Univers, découverte en 1998. L'explication théorique la plus simple repose sur l'introduction d'une constante cosmologique $Lambda$. Ce modèle, connu sous le nom de $Lambda$CDM, est en accord avec les différentes observations liées à l'expansion accélérée. Cependant, il présente des problèmes d'ordre théorique. Par conséquent, plusieurs alternatives, connues collectivement sous le nom de {it modèles d'énergie noire}, ont été proposées pour expliquer cette accélération. Plusieurs d'entre eux restent viables, car leurs {it backgrounds} cosmologiques ne présentent pas de signatures identifiables. Par contre, les effets sur les phénomènes perturbatifs sont plus spécifiques à chacun de ces modèles. Dans cette thèse, nous explorons les caractéristiques particulières de la croissance des perturbations de matière à l'ordre linéaire dans les théories $f(R)$ avec un regard complémentaire sur les modèles chameleon. La paramétrisation du taux de croissance de la matière en termes d'une fonction $gamma$ permet d'identifier une signature très spécifique de ces modèles en comparaison avec le modèle $Lambda$CDM. Une étude supplémentaire a permis de trouver une dépendance en échelle explicite, nommée {it dispersion}, dans la croissance des perturbations. Des observations plus précises pourraient permettre de faire la différence entre ces différents modèles selon la présence de ces caractéristiques. / One of the most important open issues in modern cosmology is the origin of the accelerated expansion of the Universe, observed in 1998. The simplest theoretical explanation relies on the introduction of a cosmological constant $Lambda$. This model, known as $Lambda$CDM, agrees with all the different observations connected to the accelerated expansion. However, it presents some theoretical issues. As a result, several alternatives, known collectively under the name of {it dark energy models}, have been proposed to explain this acceleration. Several among them remain viable, since their cosmological backgrounds do not show any identifiable signature. On the other hand, effects on the perturbative level are more specific to each model. In this thesis, we explore the particular characteristics of the growth of linear matter perturbations in $f(R)$ theories, with a complementary look on chameleon models. The parameterization of the growth rate in terms of a $gamma$ function allows us to identify a very specific signature of these models in comparison with the $Lambda$CDM model. A subsequent study allowed us to find an explicit scale dependance, known as {it dispersion}, in the growth of perturbations. More precise observations could enable us to distinguish between dark energy models according to the presence of this type of feature.

Experimental data suggest that the universe is homogeneous and isotropic on sufficiently large scales. An exact solution of the Einstein field equations exists for a homogeneous and isotropic universe, also known as a Friedmann-Lemaître-Robertson-Walker (FLRW) universe. However, this model is only a first approximation since we know that, locally, the universe has anisotropic and inhomogeneous structures such as galaxies and clusters of galaxies. In order to successfully introduce inhomogeneities and anisotropies to the model one uses perturbative methods. In cosmological perturbations the FLRW universe is considered the zeroth order term in a perturbation expansion and perturbation theory is used to derive higher order terms which one tries to match with observations. In this thesis I present a review of the main concepts of general relativity, discuss the 3+1 formalism which gives us the Einstein field equations in a useful form for the perturbative analysis, and lastly, I derive the first order scalar perturbations of the Einstein field equations.

In dieser Arbeit studieren wir das ekpyrotische Szenario, welches ein kosmologisches Modell des frühen Universums ist. Dieses Modell erklärt mit Hilfe einer kontrahierenden ekpyrotischen Phase die "Anfangsbedingungen" des Universums. Das bedeutet, dass der konventionelle "Urknall" durch einem Rückprall ersetzt wird. In dieser Arbeit versuchen wir Unstimmigkeiten zwischen den Vorhersagen der ekpyrotischen Modelle und den Messungen der Kosmologischen Hintergrundstrahlung des Planck Satelliten zu lösen. Den Planck Messungen zufolge sind die ursprünglichen adiabatischen Fluktuationen fast skaleninvariant und gaußverteilt. Während der ekpyrotischen Phase werden typischer Weise Flutuationen mit nicht-Gaußschen Korrekturen erzeugt. Wir schlagen zwei Ansätze vor, um diese Unstimmigkeit zu beheben. In dem nicht-minimalen entropischen Mechanismus werden fast skaleninvariante entropische Fluktuationen mit Hilfe einer nicht-minimalen kinetischen Kopplung zwischen zwei Skalarfeldern erzeugt. Wir werden zeigen, dass die nicht-Gaußschen Korrekturen während der ekpyrotischen Phase genau Null sind. Dies führt zu insgesamt kleinen nicht-Gaußschen Korrekturen nach der Umwandlung von entropischen zu adiabatischen Fluktuationen. Im Folgendem werden wir eine kinetische Umwandlung untersuchen, die nach einem nicht-singulären Rückprall stattfindet. Das Wachstum der entropischen Fluktuationen während des Rückpralls hat zur Folge, dass die möglichen nicht-Gaußschen Korrekturen, die zur Zeit der ekpyrotischen Phase erzeugt wurden, während des Rückpralls unterdrückt werden. Im letzten Teil der Arbeit gehen wir ein gravierendes Problem des inflationären Paradigmas an, welches "slow-roll eternal inflation" genannt wird. Wir schlagen ein Modell vor, das Ideen von Inflation und Ekpyrosis verbindet. Während der Konflation expandiert das Universum beschleunigt. Die adiabatischen Fluktuationen verhalten sich jedoch wie bei ekpyrotischen Modellen und wird "slow-roll eternal inflation" verhindert. / In this thesis, we study the ekpyrotic scenario, which is a cosmological model of the early universe. In this model the ``initial conditions'' of the universe are determined by a contracting ekpyrotic phase, which means that the conventional ``Big Bang'' is replaced by a bounce. The following thesis addresses the tension between ekpyrotic predictions and the observations of the Cosmic Microwave Background radiation by the Planck team. According to the Planck data, the primordial curvature fluctuations are nearly scale-invariant and Gaussian. However, during ekpyrosis, the fluctuations have typically sizable non-Gaussian signatures. In this thesis, we propose two approaches in order to resolve the tension with observations. In the non-minimal entropic mechanism, nearly scale-invariant entropy perturbations are created due to a non-minimal kinetic coupling between two scalar fields. We will show that the non-Gaussian corrections during ekpyrosis are precisely zero leading to overall small non-Gaussian signatures after the conversion process from entropy perturbations to curvature perturbations. In the following, we will consider a kinetic conversion phase, which takes place after a non-singular bounce. Due to the growth of entropy perturbations during the bounce phase, the possibly large non-Gaussian corrections created during the ekpyrotic phase become suppressed during the bounce. The last part of this thesis addresses a major problem of the inflationary paradigm: Due to large adiabatic fluctuations, slow-roll eternal inflation creates infinitely many physically distinct pocket universes. We propose a model in the framework of scalar-tensor theories, which conflated ideas of both inflation and ekpyrosis. During conflation, the universe undergoes accelerated expansion, but there are no large adiabatic fluctuations like during ekpyrosis resulting in the absence of slow-roll eternal inflation.

The identity of dark matter is one of the key outstanding problems in both particle and astrophysics. In this thesis, I describe a number of complementary searches for particle dark matter. I discuss how the impact of dark matter on stars can constrain its interaction with nuclei, focussing on main sequence stars close to the Galactic Centre, and on the first stars as seen through the upcoming James Webb Space Telescope. The mass and annihilation cross-section of dark matter particles can be probed with searches for gamma rays produced in astronomical targets. Dwarf galaxies and ultracompact, primordially-produced dark matter minihalos turn out to be especially promising in this respect. I illustrate how the results of these searches can be combined with constraints from accelerators and cosmology to produce a single global fit to all available data. Global fits in supersymmetry turn out to be quite technically demanding, even with the simplest predictive models and the addition of complementary data from a bevy of astronomical and terrestrial experiments; I show how genetic algorithms can help in overcoming these challenges. / At the time of the doctoral defense, the following papers were unpublished and had a status as follows: Paper 5: Accepted. Paper 6: Submitted.

L'expansion accélérée de l'univers est devenu un fait établi que personne ne pouvait prévoir il y a encore une vingtaine d'années. Pour expliquer l'accélération cosmique, l'univers doit être composé de $75%$ d'énergie noire, une matière hypothétique à pression négative. Une alternative aussi vertigineuse consiste à modifier la relativité générale d'Einstein à l'échelle cosmique.Mes travaux de thèse portent sur la contrainte des modèles d'énergie noire et de gravité modifiée avec les données observationnelles provenant de la croissance linéaire des structures cosmologiques. Une méthode basée sur une nouvelle paramétrisation de l'index de croissance des perturbations linéaires cosmologiques permet d'analyser un grand nombre de modèles "accélératoires" en même temps. Nous avons évalué et validé cette méthode par une analyse systématique de sa précision et de sa performance. Mes résultats montrent que le modèle standard de la cosmologie (le modèle $Lambda$CDM) reste en accord avec les données actuelles. Dans une étude approfondie, nous simulons les contraintes possibles avec les futures sondes cosmologiques de "précision" comme Euclid. Pour analyser encore plus de modèles en même temps, nous introduisons la théorie effective des champs de l'énergie noire (EFT) dans le formalisme développé auparavant. La EFT est un formalisme prometteur qui permet d'explorer d'une manière complète tous les modèles gravitationnels non-standards résultant de l'addition d'un degré de liberté supplémentaire dans l'équation d'Einstein. Nous proposons une paramétrisation de cette théorie que nous confrontons avec les données actuelles et futures. / The accelerated expansion of the universe has become an established fact that nobody could foresee until twenty years ago. To explain the cosmic acceleration, the universe must be composed by $75%$ of dark energy, a hypothetical form of matter with negative pressure. Alternatively, Einstein's field equation must be modified on cosmic scales. During my thesis I have worked on the constraint of dark energy and modified gravity models with data coming from the observed growth rate of cosmic structures. We have introduced a method based on a new parametrization of the growth index of linear cosmological perturbations. An advantage is the possibility of a concurrent analysis of multiple accelerating models. We have evaluated and validated the method in a systematic precision and performance check. My results show that the standard model of cosmology (the $Lambda$CDM model) remains consistent with current data. In an ongoing study, we have simulated future constraints for upcoming cosmological 'precision' probes like Euclid.In a second step, we introduce the effective field theory of dark energy (EFT) into our formalism. The EFT is a promising framework that allows to explore in a complete way all non-standard gravitational models that result from adding one degree of freedom in Einstein's field equation. Another advantage is its neat split of background and perturbation observables. We propose a parametrization of the EFT that we confront with current and simulated future constraints.