Testing Models of Cosmological Inflation

Total Page:16

File Type:pdf, Size:1020Kb

Testing Models of Cosmological Inflation Testing Models of Cosmological Inflation Christopher Michael Graham Thesis submitted for the degree of Doctor of Philosophy School of Mathematics and Statistics University of Newcastle upon Tyne Newcastle upon Tyne United Kingdom April 2010 Dedicated to the memory of Norah Mander. Acknowledgements This research was made possible through financial support from the Science and Technology Facilities Council and the School of Mathematics and Statistics. I’d like to say a big thank you to my fellow postgraduate students, companions on my PhD journey. From my 1st year, the M416 Merz Court crew, in particular Dave Ryan, who’s singing brightened many a gloomy afternoon and Sam James for helpful physics discussions and as a team leader in all things extra-curricular. More recently thanks to Andrew Baggaley, Stuart Cockburn (and his supervisor Nick Proukakis) for many helpful chats on thermalisation, and all of the other postgrad- uate students with whom I shared offices, borrowed books and stationary or conversed with over lunch. A big thank you to my second supervisor Andrew Fletcher who has always been available for useful discussions about my work, and to Anvar Shukurov and David Toms who stepped in to help with my viva arrangements in the last few months. Thank you to my external examiners also, Arjun Berera and Ed Copeland. A huge thank you to Antonia who endured the strains of living with me, and was always there to support me, and to my parents, my sister Catherine and my extended family. To my friends outside of academia too, particularly Andy and Darren who helped me juggle my life in recent months. And finally this thesis would not have been possible without my supervisor Ian Moss. Without Ian’s guidance, enthusiasm and seemingly infinite knowledge of the subject there would still be no end in sight and it is to him that I am most grateful. Abstract Over the past two decades cosmological inflation has become an essential ingredient to any model of the early universe. Measurements of temperature fluctuations observed in the Cosmic Microwave Background are in remarkable agreement with the predictions of inflationary models, and for the first time these results have allowed these models to be intensively tested against observational data. This thesis considers the building and testing of inflationary models which can be consistent with the Cosmic Microwave Background data. In particular the consistency of warm inflation is tested, a model where density fluctuations arise from thermal, rather than quantum vacuum fluctuations, and the possibility of distinguishing this model from standard inflationary theories is considered. The decay channels for the production of low-mass particles during standard and warm inflation are analysed to yield new results for the particle production rates. The subsequent thermalisation of particles is investigated numerically for both cases. It is concluded that in some situations the radiation produced during inflation can remain in thermal equilibrium, allowing modified inflaton equations parameterised by a single temperature-dependent friction coefficient. New results are obtained for the power spectrum of fluctuations at the end of inflation for several models of warm inflation, results that will be very important when testing temperature-dependent models against Cosmic Microwave Background data. The primordial power spectrum of fluctuations alone is not enough to distinguish between different models of inflation. The bispectrum statistic of non-Gaussianity is calculated for temperature-independent warm inflation, and for comparison the curva- ton model, to conclude that forthcoming Cosmic Microwave Background satellite data should be able to detect and distinguish any non-Gaussian signal for warm inflation from other models through its signal strength and the shape of the bispectrum. Preface This thesis is based partially upon the following papers: ”Testing Models of Inflation with CMB non-Gaussianity” • Ian G. Moss, Chris M. Graham JCAP 0711:004,2007 ”Particle Production and Reheating in the Inflationary Universe” • Ian G. Moss, Chris M. Graham Phys.Rev.D78:123526,2008 ”Density Fluctuations from Warm Inflation” • Chris M. Graham, Ian G. Moss JCAP07(2009)013 i Contents 1 Introduction 1 2 Cosmological inflation 4 2.1 Motivation for inflation . 4 2.2 Inflationarydynamics ............................ 9 2.3 Theslow-rollapproximation . 12 2.4 Reheating ................................... 13 2.5 Inflationarymodels.............................. 13 2.6 Warminflation ................................ 15 3 The source of density fluctuations 17 3.1 Comovingscales ............................... 18 3.2 Vacuum fluctuations as the source of density fluctuations ........ 18 3.3 Thermal fluctuations as the source of density fluctuations ........ 21 3.3.1 Fluctuations in the case Γ = Γ (φ) ................. 22 3.3.2 Fluctuations in the case Γ = Γ (T, φ)................ 25 3.4 Numerical simulation of coupled fluctuations . ...... 27 3.4.1 Numericalapproach . 27 3.4.2 Dependency on r and c ....................... 29 3.4.3 Dampingeffects ........................... 30 4 Reheating the universe 34 4.1 Particleproductionmethod . 35 4.1.1 Someusefuldefinitions. 35 ii Contents 4.1.2 Theparticlenumberdensity. 36 4.1.3 Theparticleproductionrate . 37 4.2 Particle production calculations . ..... 39 4.2.1 Oscillating fields by the scattering matrix method . ..... 40 4.2.2 Oscillating fields by the general method . 41 4.2.3 Particle production in the adiabatic approximation . ....... 43 4.2.4 Particle production in the 2-Stage decay model . 44 4.3 The thermalisation of particles . 46 4.3.1 Intheoscillatingphase . 49 4.3.2 Intheslow-rollphase . 50 4.3.3 Thermalisation with the full Boltzmann collision integral . 52 5 The cosmic microwave background 57 5.1 Evolution of perturbations after inflation . ....... 57 5.2 MeasurementoftheCMB . .. .. .. .. .. .. .. 59 5.3 CMBdataanalysis.............................. 60 5.4 Theangularpowerspectrum . 60 5.5 Power spectrum predictions using numerical code . ....... 63 6 Testing models of inflation with CMB non-Gaussianity 66 6.1 Quantifyingthenon-Gaussianity . 67 6.2 TheCMBbispectrum ............................ 67 6.2.1 Thecurvatonmodel ......................... 69 6.2.2 Warminflation ............................ 74 6.3 Numerical calculation of the bispectrum . ..... 74 6.4 Distinguishing between inflationary models . ...... 77 6.5 Non-Gaussianity tests on CMB data . 80 7 Conclusion 85 A Numerical methods 87 A.1 Numerical simulation of the stochastic fluctuations . ......... 87 iii Contents A.2 ModificationstoCMBFAST. 89 A.3 CalculatingtheFishermatrix . 92 B Reduction of the Collision Integral 95 C Bispectrum calculations 99 C.1 General expression for the angle-averaged bispectrum . ......... 99 C.2 Warm inflation angle-averaged bispectrum . 100 iv Chapter 1 Introduction The discovery and subsequent precise measurements of the Cosmic Microwave Back- ground (CMB) in the past two decades have transformed the subject that is Cosmo- logical Inflation. The early moments of the universe have long been studied, but it is with the measurement of the CMB that the earliest of these, the exponential expansion of the universe known as inflation at some 10−42 seconds old, can be studied in great depth. Indeed, the very title of this thesis, ’testing models of inflation’, is now a reality. It is very well known that towards the end of the Hot Big Bang, a very long time after inflation, photons and electrons in a plasma universe decouple, leaving photons to travel freely through space in the transparent universe that we see today. It is these photons released at the decoupling time, which after billions of years are observable as the microwaves of the CMB. While this is overwhelming evidence for the Hot Big Bang, even more astounding is that the imprint of inflation is left in the CMB in the form of small scale temperature anisotropies. At the onset of inflation, the universe is small enough that quantum vacuum fluctu- ations are important. Inflationary models predict that these quantum fluctuations are the seed for density fluctuations which are not only visible in the CMB temperature spectrum, but also in the distribution of large scale structure in the universe. With this snapshot of the universe at the decoupling time, measurements of the CMB are an extremely powerful tool for determining the physics of the early universe, both during inflation and beyond. Indeed, it would not be bold to say that the precise measurements of the COBE satellite in 1991 and WMAP satellite in 2001-2007 have transformed the subject of Cosmology. This thesis considers the building and testing of inflationary models which can be consistent with the CMB data. There are at present many many models that can be considered consistent and the quest now is to find a definitive model of inflation, a task 1 Chapter 1. Introduction that will require analysis after analysis of each model, and ultimately even more precise measurement of the CMB. In particular, this thesis considers the consistency of a model known as warm infla- tion, and the possibility of distinguishing this model from standard (cold) inflationary theories. In warm inflation, radiation is produced alongside the expansion of the uni- verse, which solves very neatly one, perhaps undesirable, problem of standard inflation- ary models, that the universe cools as it expands, leaving it far below the temperatures required for the Hot Big Bang to continue. In standard theories this is solved by having a separate period of reheating at
Recommended publications
  • Time-Dependent Cosmological Interpretation of Quantum Mechanics Emmanuel Moulay
    Time-dependent cosmological interpretation of quantum mechanics Emmanuel Moulay To cite this version: Emmanuel Moulay. Time-dependent cosmological interpretation of quantum mechanics. 2016. hal- 01169099v2 HAL Id: hal-01169099 https://hal.archives-ouvertes.fr/hal-01169099v2 Preprint submitted on 18 Nov 2016 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Time-dependent cosmological interpretation of quantum mechanics Emmanuel Moulay∗ Abstract The aim of this article is to define a time-dependent cosmological inter- pretation of quantum mechanics in the context of an infinite open FLRW universe. A time-dependent quantum state is defined for observers in sim- ilar observable universes by using the particle horizon. Then, we prove that the wave function collapse of this quantum state is avoided. 1 Introduction A new interpretation of quantum mechanics, called the cosmological interpre- tation of quantum mechanics, has been developed in order to take into account the new paradigm of eternal inflation [1, 2, 3]. Eternal inflation can lead to a collection of infinite open Friedmann-Lemaˆıtre-Robertson-Walker (FLRW) bub- ble universes belonging to a multiverse [4, 5, 6]. This inflationary scenario is called open inflation [7, 8].
    [Show full text]
  • Primordial Gravitational Waves and Cosmology Arxiv:1004.2504V1
    Primordial Gravitational Waves and Cosmology Lawrence Krauss,1∗ Scott Dodelson,2;3;4 Stephan Meyer 3;4;5;6 1School of Earth and Space Exploration and Department of Physics, Arizona State University, PO Box 871404, Tempe, AZ 85287 2Center for Particle Astrophysics, Fermi National Laboratory PO Box 500, Batavia, IL 60510 3Department of Astronomy and Astrophysics 4Kavli Institute of Cosmological Physics 5Department of Physics 6Enrico Fermi Institute University of Chicago, 5640 S. Ellis Ave, Chicago, IL 60637 ∗To whom correspondence should be addressed; E-mail: [email protected]. The observation of primordial gravitational waves could provide a new and unique window on the earliest moments in the history of the universe, and on possible new physics at energies many orders of magnitude beyond those acces- sible at particle accelerators. Such waves might be detectable soon in current or planned satellite experiments that will probe for characteristic imprints in arXiv:1004.2504v1 [astro-ph.CO] 14 Apr 2010 the polarization of the cosmic microwave background (CMB), or later with di- rect space-based interferometers. A positive detection could provide definitive evidence for Inflation in the early universe, and would constrain new physics from the Grand Unification scale to the Planck scale. 1 Introduction Observations made over the past decade have led to a standard model of cosmology: a flat universe dominated by unknown forms of dark energy and dark matter. However, while all available cosmological data are consistent with this model, the origin of neither the dark energy nor the dark matter is known. The resolution of these mysteries may require us to probe back to the earliest moments of the big bang expansion, but before a period of about 380,000 years, the universe was both hot and opaque to electromagnetic radiation.
    [Show full text]
  • 19. Big-Bang Cosmology 1 19
    19. Big-Bang cosmology 1 19. BIG-BANG COSMOLOGY Revised September 2009 by K.A. Olive (University of Minnesota) and J.A. Peacock (University of Edinburgh). 19.1. Introduction to Standard Big-Bang Model The observed expansion of the Universe [1,2,3] is a natural (almost inevitable) result of any homogeneous and isotropic cosmological model based on general relativity. However, by itself, the Hubble expansion does not provide sufficient evidence for what we generally refer to as the Big-Bang model of cosmology. While general relativity is in principle capable of describing the cosmology of any given distribution of matter, it is extremely fortunate that our Universe appears to be homogeneous and isotropic on large scales. Together, homogeneity and isotropy allow us to extend the Copernican Principle to the Cosmological Principle, stating that all spatial positions in the Universe are essentially equivalent. The formulation of the Big-Bang model began in the 1940s with the work of George Gamow and his collaborators, Alpher and Herman. In order to account for the possibility that the abundances of the elements had a cosmological origin, they proposed that the early Universe which was once very hot and dense (enough so as to allow for the nucleosynthetic processing of hydrogen), and has expanded and cooled to its present state [4,5]. In 1948, Alpher and Herman predicted that a direct consequence of this model is the presence of a relic background radiation with a temperature of order a few K [6,7]. Of course this radiation was observed 16 years later as the microwave background radiation [8].
    [Show full text]
  • Contribution Prospectives 2020 Cosmology with Gravitational Waves
    Contribution Prospectives 2020 Cosmology with Gravitational Waves Principal author: D.A. Steer Co-authors: V. Vennin, D. Langlois, K. Noui, F. Nitti, E. Kiritsis, M. Khlopov, E. Huguet (Theory group at APC) Virgo groups at APC, ARTEMIS, ILM, IPHC, IP2I, LAL, LAPP and LKB Abstract Gravitational waves, which were detected directly for the first time by the LIGO-Virgo scientific collaboration, can be used to probe early and late-time cosmology. In this letter we present different aspects of research in the areas of cosmology which we believe will be of crucial importance in the next 10 years: 1) measurements of cosmological parameters with GWs; 2) early universe cosmology with GWs. This letter is supplemented by the companion \Testing General Relativity and modified gravity with Gravitational Waves". Overview The Standard Cosmological model, also referred as ΛCDM, is a highly successful model of the universe, whose predictions have passed many precise observational tests in both the early and late-time universe. Despite that, there remain a number of open questions. One, for instance, pertains to the expansion rate of the universe today | namely the Hubble constant H0 | which is a fundamental parameter of the ΛCDM. Indeed, today there is a 4:2σ discrepancy between −1 −1 the value of H0 = 66:93 ± 0:62 ; kmMpc s inferred by the Planck collaboration from Cosmic −1 −1 Microwave Background (CMB) and the value of H0 = 73:5 ± 1:4 kmMpc s measured from Type Ia Supernovae. A recent improvement of the latter estimation method (using extended HST observations of Cepheids in the LMC) leads to the even larger discrepancy of 4:4σ [1].
    [Show full text]
  • Different Horizons in Cosmology
    Horizons in Cosmology Robert D. Klauber www.quantumfieldtheory.info October 9, 2018 Refs: Davis, T.M., and Lineweaver, C.H., Expanding Confusion: common misconceptions of cosmological horizons and the superluminal expansion of the universe, https://arxiv.org/abs/astro-ph/0310808 Melia, F., The apparent (gravitational) horizon in cosmology, Am. J. Phys. ¸86 (8), Aug 2018, pgs. 585-593. https://arxiv.org/abs/1807.07587 Wholeness Chart in Words: Cosmological Horizons Value Now Type Decelerating Accelerating (light-years Horizon Universe Universe Note in billions) Hubble LH = radius at which As at left Function of time. 14.3 sphere galaxy recession velocity = c Function of time, but Particle LP = distance to common meaning is now As at left 46 horizon farthest light we (our present time). can see This = observable universe LE = distance from us now at which we will never see light emitted from there now Function of time (i.e., function of what time we Not exist for Also = distance from us now at which Event take as “now”). eternally slowing light we emit now will never be seen by 16 horizon expansion. any observer there. Acceleration moves distant space away faster Also = distance now to the farthest than light can reach it. location we could ever reach if we left now at speed of light. Mathematics of Cosmological Horizons 1 The Universe’s Metric and Physical Distances The Friedmann–Lemaître–Robertson–Walker metric for a homogeneous, isotropic universe is 2222 22 2 ds cdt at d Sk d (1) where a(t) is the expansion factor of the universe at time t, is the comoving radial coordinate where we can take Earth at = 0, present time is t0, a(t0) = 1, and Sk depends on the curvature of the 3D spatial universe, i.e.
    [Show full text]
  • Big-Bang Cosmology 1 21
    21. Big-Bang cosmology 1 21. Big-Bang Cosmology Revised September 2017 by K.A. Olive (University of Minnesota) and J.A. Peacock (University of Edinburgh). 21.1. Introduction to Standard Big-Bang Model The observed expansion of the Universe [1–3] is a natural (almost inevitable) result of any homogeneous and isotropic cosmological model based on general relativity. However, by itself, the Hubble expansion does not provide sufficient evidence for what we generally refer to as the Big-Bang model of cosmology. While general relativity is in principle capable of describing the cosmology of any given distribution of matter, it is extremely fortunate that our Universe appears to be homogeneous and isotropic on large scales. Together, homogeneity and isotropy allow us to extend the Copernican Principle to the Cosmological Principle, stating that all spatial positions in the Universe are essentially equivalent. The formulation of the Big-Bang model began in the 1940s with the work of George Gamow and his collaborators, Alpher and Herman. In order to account for the possibility that the abundances of the elements had a cosmological origin, they proposed that the early Universe which was once very hot and dense (enough so as to allow for the nucleosynthetic processing of hydrogen), and has expanded and cooled to its present state [4,5]. In 1948, Alpher and Herman predicted that a direct consequence of this model is the presence of a relic background radiation with a temperature of order a few K [6,7]. Of course this radiation was observed 16 years later as the microwave background radiation [8].
    [Show full text]
  • Black Hole Versus Cosmological Horizon Entropy 2
    Black hole versus cosmological horizon entropy Tamara M. Davis, P. C. W. Davies & Charles H. Lineweaver Abstract. The generalized second law of thermodynamics states that entropy always increases when all event horizons are attributed with an entropy proportional to their area. We test the generalized second law by investigating the change in entropy when dust, radiation and black holes cross a cosmological event horizon. We generalize for flat, open and closed Friedmann-Robertson-Walker universes by using numerical calculations to determine the cosmological horizon evolution. In most cases the loss of entropy from within the cosmological horizon is more than balanced by an increase in cosmological event horizon entropy, maintaining the validity of the generalized second law of thermodynamics. However, an intriguing set of open universe models show an apparent entropy decrease when black holes disappear over the cosmological event horizon. We anticipate that this apparent violation of the generalized second law will disappear when solutions are available for black holes embedded in arbitrary backgrounds. PACS numbers: 04.70.Dy, 98.80.Jk, 02.60.Jh, 04.20.Cv arXiv:astro-ph/0305121v2 21 Aug 2003 Black hole versus cosmological horizon entropy 2 1. Introduction A significant advance in physical theory was made by Bekenstein with the suggestion (Bekenstein 1970) that the area of the event horizon of a black hole is a measure of its entropy. This hinted at a deep link between information, gravitation and quantum mechanics that remains tantalizingly unresolved today. Bekenstein’s claim was bolstered by Hawking’s application of quantum field theory to black holes (Hawking 1975), from which he deduced that these objects emit thermal radiation with a characteristic temperature, 1 Tb = , (1) 8πmb for a Schwarzschild hole, where mb is the mass of the black hole, and we use units G =¯h = c = k = 1.
    [Show full text]
  • Lectures on Astronomy, Astrophysics, and Cosmology
    Lectures on Astronomy, Astrophysics, and Cosmology Luis A. Anchordoqui Department of Physics and Astronomy, Lehman College, City University of New York, NY 10468, USA Department of Physics, Graduate Center, City University of New York, 365 Fifth Avenue, NY 10016, USA Department of Astrophysics, American Museum of Natural History, Central Park West 79 St., NY 10024, USA (Dated: Spring 2016) I. STARS AND GALAXIES minute = 1:8 107 km, and one light year × 1 ly = 9:46 1015 m 1013 km: (1) A look at the night sky provides a strong impression of × ≈ a changeless universe. We know that clouds drift across For specifying distances to the Sun and the Moon, we the Moon, the sky rotates around the polar star, and on usually use meters or kilometers, but we could specify longer times, the Moon itself grows and shrinks and the them in terms of light. The Earth-Moon distance is Moon and planets move against the background of stars. 384,000 km, which is 1.28 ls. The Earth-Sun distance Of course we know that these are merely local phenomena is 150; 000; 000 km; this is equal to 8.3 lm. Far out in the caused by motions within our solar system. Far beyond solar system, Pluto is about 6 109 km from the Sun, or 4 × the planets, the stars appear motionless. Herein we are 6 10− ly. The nearest star to us, Proxima Centauri, is going to see that this impression of changelessness is il- about× 4.2 ly away. Therefore, the nearest star is 10,000 lusory.
    [Show full text]
  • Natural Observer Fields and Redshift 1 Introduction
    Natural observer fields and redshift ROBERT SMACKAY COLIN ROURKE We sketch the construction of space-times with observer fields which have redshift satisfying Hubble’s law but no big bang. 83F05; 83C15, 83C40, 83C57 1 Introduction This paper is part of a program whose aim is to establish a new paradigm for the universe in which there is no big bang. There are three pieces of primary evidence for the big bang: the distribution of light elements, the cosmic microwave background, and redshift. This paper concentrates on redshift. Alternative explanations for the other pieces of primary evidence are given in other papers in the program. The context for our investigation of redshift is the concept of an observer field by which we mean a future-pointing time-like unit vector field. An observer field is natural if the integral curves (field lines) are geodesic and the perpendicular 3–plane field is integrable (giving normal space slices). It then follows that the field determines a local coherent notion of time: a time coordinate that is constant on the perpendicular space slices and whose difference between two space slices is the proper time along any field line. This is proved in [6, Section 5]. In a natural observer field, red or blueshift can be measured locally and corresponds precisely to expansion or contraction of space measured in the direction of the null geodesic being considered (this is proved in Section 2 of this paper). Therefore, if one assumes the existence of a global natural observer field, an assumption made implicitly in current conventional cosmology, then redshift leads directly to global expansion and the big bang.
    [Show full text]
  • 22. Big-Bang Cosmology
    1 22. Big-Bang Cosmology 22. Big-Bang Cosmology Revised August 2019 by K.A. Olive (Minnesota U.) and J.A. Peacock (Edinburgh U.). 22.1 Introduction to Standard Big-Bang Model The observed expansion of the Universe [1–3] is a natural (almost inevitable) result of any homogeneous and isotropic cosmological model based on general relativity. However, by itself, the Hubble expansion does not provide sufficient evidence for what we generally refer to as the Big-Bang model of cosmology. While general relativity is in principle capable of describing the cosmology of any given distribution of matter, it is extremely fortunate that our Universe appears to be homogeneous and isotropic on large scales. Together, homogeneity and isotropy allow us to extend the Copernican Principle to the Cosmological Principle, stating that all spatial positions in the Universe are essentially equivalent. The formulation of the Big-Bang model began in the 1940s with the work of George Gamow and his collaborators, Ralph Alpher and Robert Herman. In order to account for the possibility that the abundances of the elements had a cosmological origin, they proposed that the early Universe was once very hot and dense (enough so as to allow for the nucleosynthetic processing of hydrogen), and has subsequently expanded and cooled to its present state [4,5]. In 1948, Alpher and Herman predicted that a direct consequence of this model is the presence of a relic background radiation with a temperature of order a few K [6,7]. Of course this radiation was observed 16 years later as the Cosmic Microwave Background (CMB) [8].
    [Show full text]
  • A Model of Nonsingular Universe
    Entropy 2012, 14, 1296-1305; doi:10.3390/e14071296 OPEN ACCESS entropy ISSN 1099-4300 www.mdpi.com/journal/entropy Article A Model of Nonsingular Universe Changjun Gao 1;2 1 The National Astronomical Observatories, Chinese Academy of Sciences, Beijing 100012, China; E-Mail: [email protected] 2 Kavli Institute for Theoretical Physics China, CAS, Beijing 100190, China Received: 19 April 2012; in revised form: 4 June 2012 / Accepted: 13 June 2012 / Published: 23 July 2012 Abstract: In the background of Friedmann–Robertson–Walker Universe, there exists Hawking radiation which comes from the cosmic apparent horizon due to quantum effect. Although the Hawking radiation on the late time evolution of the universe could be safely neglected, it plays an important role in the very early stage of the universe. In view of this point, we identify the temperature in the scalar field potential with the Hawking temperature of cosmic apparent horizon. Then we find a nonsingular universe sourced by the temperature-dependent scalar field. We find that the universe could be created from a de Sitter phase which has the Planck energy density. Thus the Big-Bang singularity is avoided. Keywords: Hawking temperature; scalar field; nonsingular universe 1. Introduction The standard model of cosmology claims that the primordial Universe was in a hot, dense, and highly curved state which is very close to the Big-Bang singularity [1]. The cosmic energy density, the temperature and other physical quantities become infinite at the singularity. Thus the presence of infinity of physical quantities indicates that the Einstein’s General Relativity breaks down at the singularity.
    [Show full text]
  • Topics in Cosmology: Island Universes, Cosmological Perturbations and Dark Energy
    TOPICS IN COSMOLOGY: ISLAND UNIVERSES, COSMOLOGICAL PERTURBATIONS AND DARK ENERGY by SOURISH DUTTA Submitted in partial fulfillment of the requirements for the degree Doctor of Philosophy Department of Physics CASE WESTERN RESERVE UNIVERSITY August 2007 CASE WESTERN RESERVE UNIVERSITY SCHOOL OF GRADUATE STUDIES We hereby approve the dissertation of ______________________________________________________ candidate for the Ph.D. degree *. (signed)_______________________________________________ (chair of the committee) ________________________________________________ ________________________________________________ ________________________________________________ ________________________________________________ ________________________________________________ (date) _______________________ *We also certify that written approval has been obtained for any proprietary material contained therein. To the people who have believed in me. Contents Dedication iv List of Tables viii List of Figures ix Abstract xiv 1 The Standard Cosmology 1 1.1 Observational Motivations for the Hot Big Bang Model . 1 1.1.1 Homogeneity and Isotropy . 1 1.1.2 Cosmic Expansion . 2 1.1.3 Cosmic Microwave Background . 3 1.2 The Robertson-Walker Metric and Comoving Co-ordinates . 6 1.3 Distance Measures in an FRW Universe . 11 1.3.1 Proper Distance . 12 1.3.2 Luminosity Distance . 14 1.3.3 Angular Diameter Distance . 16 1.4 The Friedmann Equation . 18 1.5 Model Universes . 21 1.5.1 An Empty Universe . 22 1.5.2 Generalized Flat One-Component Models . 22 1.5.3 A Cosmological Constant Dominated Universe . 24 1.5.4 de Sitter space . 26 1.5.5 Flat Matter Dominated Universe . 27 1.5.6 Curved Matter Dominated Universe . 28 1.5.7 Flat Radiation Dominated Universe . 30 1.5.8 Matter Radiation Equality . 32 1.6 Gravitational Lensing . 34 1.7 The Composition of the Universe .
    [Show full text]