Inhomogeneous Cosmology in an Anisotropic Universe
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Inhomogeneous Cosmology with Numerical Relativity
PHYSICAL REVIEW D 95, 064028 (2017) Inhomogeneous cosmology with numerical relativity Hayley J. Macpherson,* Paul D. Lasky, and Daniel J. Price Monash Centre for Astrophysics and School of Physics and Astronomy, Monash University, Clayton, Victoria 3800, Australia (Received 16 November 2016; published 17 March 2017) We perform three-dimensional numerical relativity simulations of homogeneous and inhomogeneous expanding spacetimes, with a view toward quantifying nonlinear effects from cosmological inhomoge- neities. We demonstrate fourth-order convergence with errors less than one part in 106 in evolving a flat, dust Friedmann-Lemaître-Roberston-Walker spacetime using the Einstein Toolkit within the Cactus framework. We also demonstrate agreement to within one part in 103 between the numerical relativity solution and the linear solution for density, velocity and metric perturbations in the Hubble flow over a factor of ∼350 change in scale factor (redshift). We simulate the growth of linear perturbations into the nonlinear regime, where effects such as gravitational slip and tensor perturbations appear. We therefore show that numerical relativity is a viable tool for investigating nonlinear effects in cosmology. DOI: 10.1103/PhysRevD.95.064028 I. INTRODUCTION spacetimes [41], the propagation and collision of gravita- tional wave perturbations [42,43] and linearized perturba- Modern cosmology relies on the cosmological principle— tions to a homogeneous spacetime [44,45]. More recent that the Universe is sufficiently homogeneous and isotropic work has continued to include symmetries to simplify the on large scales to be described by a Friedmann-Lemaître- numerical calculations, e.g. Refs. [46,47]. Robertson-Walker (FLRW) model. Cosmological N-body Simulations free of these symmetries have only emerged simulations, e.g. -
On Gravitational Energy in Newtonian Theories
On Gravitational Energy in Newtonian Theories Neil Dewar Munich Center for Mathematical Philosophy LMU Munich, Germany James Owen Weatherall Department of Logic and Philosophy of Science University of California, Irvine, USA Abstract There are well-known problems associated with the idea of (local) gravitational energy in general relativity. We offer a new perspective on those problems by comparison with Newto- nian gravitation, and particularly geometrized Newtonian gravitation (i.e., Newton-Cartan theory). We show that there is a natural candidate for the energy density of a Newtonian gravitational field. But we observe that this quantity is gauge dependent, and that it cannot be defined in the geometrized (gauge-free) theory without introducing further structure. We then address a potential response by showing that there is an analogue to the Weyl tensor in geometrized Newtonian gravitation. 1. Introduction There is a strong and natural sense in which, in general relativity, there are metrical de- grees of freedom|including purely gravitational, i.e., source-free degrees of freedom, such as gravitational waves|that can influence the behavior of other physical systems. And yet, if one attempts to associate a notion of local energy density with these metrical degrees of freedom, one quickly encounters (well-known) problems.1 For instance, consider the following simple argument that there cannot be a smooth ten- Email address: [email protected] (James Owen Weatherall) 1See, for instance, Misner et al. (1973, pp. 466-468), for a classic argument that there cannot be a local notion of energy associated with gravitation in general relativity; see also Choquet-Brouhat (1983), Goldberg (1980), and Curiel (2017) for other arguments and discussion. -
Spectral Distortion in a Radially Inhomogeneous Cosmology
Dartmouth College Dartmouth Digital Commons Dartmouth Scholarship Faculty Work 11-5-2013 Spectral Distortion in a Radially Inhomogeneous Cosmology R. R. Caldwell Dartmouth College N. A. Maksimova Dartmouth College Follow this and additional works at: https://digitalcommons.dartmouth.edu/facoa Part of the Cosmology, Relativity, and Gravity Commons Dartmouth Digital Commons Citation Caldwell, R. R. and Maksimova, N. A., "Spectral Distortion in a Radially Inhomogeneous Cosmology" (2013). Dartmouth Scholarship. 1962. https://digitalcommons.dartmouth.edu/facoa/1962 This Article is brought to you for free and open access by the Faculty Work at Dartmouth Digital Commons. It has been accepted for inclusion in Dartmouth Scholarship by an authorized administrator of Dartmouth Digital Commons. For more information, please contact [email protected]. Spectral Distortion in a Radially Inhomogeneous Cosmology R. R. Caldwell1 and N. A. Maksimova1 1Department of Physics & Astronomy, Dartmouth College, 6127 Wilder Laboratory, Hanover, NH 03755 USA (Dated: October 16, 2013) The spectral distortion of the cosmic microwave background blackbody spectrum in a radially inhomogeneous spacetime, designed to exactly reproduce a ΛCDM expansion history along the past light cone, is shown to exceed the upper bound established by COBE-FIRAS by a factor of approximately 3700. This simple observational test helps uncover a slew of pathological features that lie hidden inside the past light cone, including a radially contracting phase at decoupling and, if followed to its logical extreme, a naked singularity at the radially inhomogeneous Big Bang. I. INTRODUCTION Is the Universe playing fair with us? Are the laws of physics and the structure of space-time the same everywhere? It is a fundamental tenet of the Standard Cosmological Model that the answer is yes. -
Exact and Perturbed Friedmann-Lemaıtre Cosmologies
Exact and Perturbed Friedmann-Lemaˆıtre Cosmologies by Paul Ullrich A thesis presented to the University of Waterloo in fulfilment of the thesis requirement for the degree of Master of Mathematics in Applied Mathematics Waterloo, Ontario, Canada, 2007 °c Paul Ullrich 2007 I hereby declare that I am the sole author of this thesis. This is a true copy of the thesis, including any required final revisions, as accepted by my examiners. I understand that my thesis may be made electronically available to the public. ii Abstract In this thesis we first apply the 1+3 covariant description of general relativity to analyze n-fluid Friedmann- Lemaˆıtre (FL) cosmologies; that is, homogeneous and isotropic cosmologies whose matter-energy content consists of n non-interacting fluids. We are motivated to study FL models of this type as observations sug- gest the physical universe is closely described by a FL model with a matter content consisting of radiation, dust and a cosmological constant. Secondly, we use the 1 + 3 covariant description to analyse scalar, vec- tor and tensor perturbations of FL cosmologies containing a perfect fluid and a cosmological constant. In particular, we provide a thorough discussion of the behaviour of perturbations in the physically interesting cases of a dust or radiation background. iii Acknowledgements First and foremost, I would like to thank Dr. John Wainwright for his patience, guidance and support throughout the preparation of this thesis. I also would like to thank Dr. Achim Kempf and Dr. C. G. Hewitt for their time and comments. iv Contents 1 Introduction 1 1.1 Cosmological Models . -
The Local Value of H0 in an Inhomogeneous Universe
Prepared for submission to JCAP The local value of H0 in an inhomogeneous universe I. Odderskov,a S. M. Koksbang,a S. Hannestad,a aDepartment of Physics and Astronomy University of Aarhus, Ny Munkegade, Aarhus C, Denmark E-mail: [email protected], [email protected], [email protected] Abstract. The effects of local inhomogeneities on low redshift H0 determinations are studied by estimating the redshift-distance relation of mock sources in N-body simulations. The results are compared to those obtained using the standard approach based on Hubble's law. The comparison shows a clear tendency for the standard approach to yield lower values of H0 than the approach based on the scheme using light rays. The difference is, however, small. More precisely, it is found that the overall effect of inhomogeneities on the determination of H0 is a small increase in the local estimates of about 0:3% compared to the results obtained with Hubble's law, when based on a typical distribution of supernovae in the redshift range 0:01 < z < 0:1. The overall conclusion of the study is a verification of the results that have earlier been obtained by using Hubble's law: The effects of inhomogeneities on local H0 estimates are not significant enough to make it plausible that differences in high- and low-redshift estimates of H0 are due to small inhomogeneities within the setting of standard cosmology. arXiv:1601.07356v2 [astro-ph.CO] 28 Jan 2016 Contents 1 Introduction1 2 Method for computing redshift-distance relations in N-body simulations at low redshift2 3 Mock observations4 3.1 Redshift distribution of sources4 3.2 Observers5 3.3 Lightcone snapshots6 3.4 Summary6 4 Results and discussion7 5 Summary 10 6 Acknowledgments 10 1 Introduction Overall, the ΛCDM model is consistent with observations at a remarkable level considering the model's simplicity compared to the real, inhomogeneous universe. -
Physics of the Cosmic Microwave Background Anisotropy∗
Physics of the cosmic microwave background anisotropy∗ Martin Bucher Laboratoire APC, Universit´eParis 7/CNRS B^atiment Condorcet, Case 7020 75205 Paris Cedex 13, France [email protected] and Astrophysics and Cosmology Research Unit School of Mathematics, Statistics and Computer Science University of KwaZulu-Natal Durban 4041, South Africa January 20, 2015 Abstract Observations of the cosmic microwave background (CMB), especially of its frequency spectrum and its anisotropies, both in temperature and in polarization, have played a key role in the development of modern cosmology and our understanding of the very early universe. We review the underlying physics of the CMB and how the primordial temperature and polarization anisotropies were imprinted. Possibilities for distinguish- ing competing cosmological models are emphasized. The current status of CMB ex- periments and experimental techniques with an emphasis toward future observations, particularly in polarization, is reviewed. The physics of foreground emissions, especially of polarized dust, is discussed in detail, since this area is likely to become crucial for measurements of the B modes of the CMB polarization at ever greater sensitivity. arXiv:1501.04288v1 [astro-ph.CO] 18 Jan 2015 1This article is to be published also in the book \One Hundred Years of General Relativity: From Genesis and Empirical Foundations to Gravitational Waves, Cosmology and Quantum Gravity," edited by Wei-Tou Ni (World Scientific, Singapore, 2015) as well as in Int. J. Mod. Phys. D (in press). -
Inhomogeneous Cosmological Models and Averaging in Cosmology: Overview
Home Search Collections Journals About Contact us My IOPscience Inhomogeneous cosmological models and averaging in cosmology: overview This article has been downloaded from IOPscience. Please scroll down to see the full text article. 2011 Class. Quantum Grav. 28 160301 (http://iopscience.iop.org/0264-9381/28/16/160301) View the table of contents for this issue, or go to the journal homepage for more Download details: IP Address: 194.94.224.254 The article was downloaded on 11/01/2012 at 09:53 Please note that terms and conditions apply. IOP PUBLISHING CLASSICAL AND QUANTUM GRAVITY Class. Quantum Grav. 28 (2011) 160301 (7pp) doi:10.1088/0264-9381/28/16/160301 EDITORIAL Inhomogeneous cosmological models and averaging in cosmology: overview 1. Introduction Cosmological observational data [1]1, when fitted using models based on the assumption of a spatially homogeneous and isotropic Friedmann–Lemaˆıtre–Robertson–Walker (FLRW) model plus small perturbations, are usually interpreted as implying that the spatial geometry is flat, there is currently an accelerated expansion and the majority of the matter in the Universe is dark, non-baryonic and cold, giving rise to the so-called CDM-concordance model (where the dark energy is interpreted as a positive cosmological constant ). The concordance model of cosmology is now operating on a well-established and tightly constrained empirical basis. However, although the concordance CDM model is remarkably successful, there does exist significant tensions between the data and the model [2]. Furthermore, if our Universe is not a perturbation of an exact flat FLRW solution, the conventional data analyses and their interpretation are not necessarily valid [3]. -
Observational Cosmology - 30H Course 218.163.109.230 Et Al
Observational cosmology - 30h course 218.163.109.230 et al. (2004–2014) PDF generated using the open source mwlib toolkit. See http://code.pediapress.com/ for more information. PDF generated at: Thu, 31 Oct 2013 03:42:03 UTC Contents Articles Observational cosmology 1 Observations: expansion, nucleosynthesis, CMB 5 Redshift 5 Hubble's law 19 Metric expansion of space 29 Big Bang nucleosynthesis 41 Cosmic microwave background 47 Hot big bang model 58 Friedmann equations 58 Friedmann–Lemaître–Robertson–Walker metric 62 Distance measures (cosmology) 68 Observations: up to 10 Gpc/h 71 Observable universe 71 Structure formation 82 Galaxy formation and evolution 88 Quasar 93 Active galactic nucleus 99 Galaxy filament 106 Phenomenological model: LambdaCDM + MOND 111 Lambda-CDM model 111 Inflation (cosmology) 116 Modified Newtonian dynamics 129 Towards a physical model 137 Shape of the universe 137 Inhomogeneous cosmology 143 Back-reaction 144 References Article Sources and Contributors 145 Image Sources, Licenses and Contributors 148 Article Licenses License 150 Observational cosmology 1 Observational cosmology Observational cosmology is the study of the structure, the evolution and the origin of the universe through observation, using instruments such as telescopes and cosmic ray detectors. Early observations The science of physical cosmology as it is practiced today had its subject material defined in the years following the Shapley-Curtis debate when it was determined that the universe had a larger scale than the Milky Way galaxy. This was precipitated by observations that established the size and the dynamics of the cosmos that could be explained by Einstein's General Theory of Relativity. -
Cosmological Perturbations Power Spectrum Vector Perturbations Tensor Perturbations
Theoretical cosmology David Wands Homogeneous cosmology Perturbation Theoretical cosmology theory Scalar perturbations Fourier transforms Cosmological perturbations Power spectrum Vector perturbations Tensor perturbations Metric David Wands perturbations Geometrical interpretation Gauge dependence Institute of Cosmology and Gravitation Particular gauges Conformal University of Portsmouth Newtonian/Longitudinal gauge Uniform-density gauge Equating gauge-invariant 5th Tah Poe School on Cosmology variables Einstein equations Einstein equations in an arbitrary gauge Recovering Newtonian fluid equations Redshift-space distortions Recovering Newtonian fluid equations Standard model of structure formation primordial perturbations in cosmic microwave background gravitational instability large-scale structure of our Universe new observational data offers precision tests of • cosmological parameters • the nature of the primordial perturbations Inflation: initial false vacuum state drives accelerated expansion zero-point fluctuations yield spectrum of perturbations Theoretical References cosmology David Wands Homogeneous cosmology Perturbation theory Scalar perturbations I Malik and Wands, Phys Rep 475, 1 (2009), Fourier transforms Power spectrum arXiv:0809.4944 Vector perturbations Tensor perturbations I Bardeen, Phys Rev D22, 1882 (1980) Metric perturbations I Kodama and Sasaki, Prog Theor Phys Supp 78, 1 Geometrical interpretation Gauge dependence (1984) Particular gauges Conformal Bassett, Tsujikawa and Wands, Rev Mod Phys (2005), Newtonian/Longitudinal -
Observational Tests of Backreaction with Recent Data
Journal of Cosmology and Astroparticle Physics Related content - Tension in the void: cosmic rulers strain Observational tests of backreaction with recent inhomogeneous cosmologies Miguel Zumalacárregui, Juan García- data Bellido and Pilar Ruiz-Lapuente - The cosmic microwave background in an inhomogeneous universe To cite this article: Matteo Chiesa et al JCAP12(2014)049 Chris Clarkson and Marco Regis - Testing the void against cosmological data: fitting CMB, BAO, SN and H0 Tirthabir Biswas, Alessio Notari and Wessel Valkenburg View the article online for updates and enhancements. Recent citations - The background Friedmannian Hubble constant in relativistic inhomogeneous cosmology and the age of the Universe Boudewijn F. Roukema et al - Averaged Lemaître–Tolman–Bondi dynamics Eddy G Chirinos Isidro et al - Angular distribution of cosmological parameters as a probe of space-time inhomogeneities C. Sofia Carvalho and Katrine Marques This content was downloaded from IP address 131.169.4.70 on 28/11/2017 at 11:25 ournal of Cosmology and Astroparticle Physics JAn IOP and SISSA journal Observational tests of backreaction with recent data JCAP12(2014)049 Matteo Chiesa,a,b Davide Mainoa and Elisabetta Majerottoc,b aUniversity of Milan, Physics Department, via Giovanni Celoria 16, Milan, Italy bINAF-Osservatorio Astronomico di Brera, via Emilio Bianchi 46, Merate, Italy cDepartamento de F´ısica Te´orica and Instituto de F´ısica Te´orica, Universidad Aut´onoma de Madrid IFT-UAM/CSIC, 28049 Cantoblanco, Madrid, Spain E-mail: [email protected], [email protected], [email protected] Received June 3, 2014 Revised November 7, 2014 Accepted November 28, 2014 Published December 22, 2014 Abstract. -
Gauge Independence of Induced Gravitational Waves
View metadata, citation and similar papers at core.ac.uk brought to you by CORE PHYSICAL REVIEW D 101, 023523 (2020) provided by IBS Publications Repository Gauge independence of induced gravitational waves Keisuke Inomata1,2 and Takahiro Terada 3 1ICRR, University of Tokyo, Kashiwa 277-8582, Japan 2Kavli IPMU (WPI), UTIAS, University of Tokyo, Kashiwa 277-8583, Japan 3Center for Theoretical Physics of the Universe, Institute for Basic Science (IBS), Daejeon 34126, Korea (Received 10 December 2019; published 28 January 2020) We study gauge (in)dependence of the gravitational waves (GWs) induced from curvature perturbations. For the GWs produced in a radiation-dominated era, we find that the observable (late-time) GWs in the transverse-traceless (synchronous) gauge and in the Newtonian gauge are the same in contrast to a claim in the literature. We also mention the interpretation of the gauge dependence of the tensor perturbations which appears in the context of the induced GWs. DOI: 10.1103/PhysRevD.101.023523 I. INTRODUCTION determine or constrain the amplitude of the small-scale perturbations. One of the main predictions of cosmological inflation is In contrast to the linear perturbation theory, the the generation of the cosmic perturbations. So far, there is second-order (induced) tensor perturbations are known only an upper bound on the amplitude of tensor pertur- to have gauge dependence. A large change of the bation, but that of scalar perturbations, namely the power spectrum of the tensor perturbations induced in curvature perturbations, has been well established by a matter-dominated (MD) era was reported in Ref. [35]. -
Systematics of Adiabatic Modes: Flat Universes
Prepared for submission to JCAP Systematics of Adiabatic Modes: Flat Universes E. Pajer,a S. Jazayeria,b aInstitute for Theoretical Physics and Center for Extreme Matter and Emergent Phenomena, Utrecht University, Princetonplein 5, 3584 CC Utrecht, The Netherlands bSchool of Astronomy, Institute for Research in Fundamental Sciences (IPM) P. O. Box 19395-5531, Tehran, Iran E-mail: [email protected], [email protected] Abstract. Adiabatic modes are cosmological perturbations that are locally indistinguishable from a (large) change of coordinates. At the classical level, they provide model independent solutions. At the quantum level, they lead to soft theorems for cosmological correlators. We present a systematic derivation of adiabatic modes in spatially-flat cosmological backgrounds with asymptotically-perfect fluids. We find several new adiabatic modes including vector, time-dependent tensor and time-dependent scalar modes. The new vector and tensor modes decay with time in standard cosmologies but are the leading modes in contracting universes. We present a preliminary derivation of the related soft theorems. In passing, we discuss a distinction between classical and quantum adiabatic modes, we clarify the subtle nature of Weinberg’s second adiabatic mode and point out that the adiabatic nature of a perturbation is a gauge dependent statement. arXiv:1710.02177v3 [astro-ph.CO] 26 Jan 2019 Contents 1 Introduction 1 2 Newtonian Gauge 3 2.1 Known adiabatic modes 6 2.2 New adiabatic modes 9 3 Comoving gauge 15 4 Properties of adiabatic modes 17 4.1 New