Theory Development in Early Universe Cosmology

Total Page:16

File Type:pdf, Size:1020Kb

Theory Development in Early Universe Cosmology APPROACHING THE ABSOLUTE ZERO OF TIME: THEORY DEVELOPMENT IN EARLY UNIVERSE COSMOLOGY by Christopher Joel Smeenk B.A., Physics and Philosophy, Yale University, 1995 M.S., Physics and Astronomy, University of Pittsburgh, 2001 M.A., Philosophy, University of Pittsburgh, 2002 Submitted to the Graduate Faculty of Arts and Sciences in partial fulfillment of the requirements for the degree of Doctor of Philosophy University of Pittsburgh 2003 We approve the thesis of Christopher Joel Smeenk. Date of Signature John S. Earman University Professor of History and Philosophy of Science Co-Chair of Committee John D. Norton Professor of History and Philosophy of Science Chair of the Department of History and Philosophy of Science Co-Chair of Committee Laura M. Ruetsche Associate Professor of Philosophy Allen I. Janis Professor Emeritus of Physics and Astronomy iii Abstract This dissertation gives an original account of the historical development of modern cos- mology along with a philosophical assessment of related methodological and foundational is- sues. After briefly reviewing the groundbreaking work by Einstein and others, I turn to the development of early universe cosmology following the discovery of the microwave background radiation in 1965. This discovery encouraged consolidation and refinement of the big bang model, but cosmologists also noted that cosmological models could accomodate observations only at the cost of several “unnatural” assumptions regarding the initial state. I describe various attempts to eliminate initial conditions in the late 60s and early 70s, leading up to the idea that came to dominate the field: inflationary cosmology. I discuss the pre-history of inflationary cos- mology and the early development of the idea, including the account of structure formation and the introduction of the “inflaton” field. The second part of my thesis focuses on methodological issues in cosmology, opening with a discussion of three principles and their role in cosmology: the cosmological principle, indifference principle, and anthropic principle. I assess appeals to explanatory adequacy as grounds for theory choice in cosmology, and close with a discussion of confirmation theory and the issue of novelty in relation to cosmological theories. iv Table of Contents List of Figures : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : vi Acknowledgments : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : vii Chapter 1. Introduction : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 1 1.1 Einstein and Cosmology . 2 1.2 Evolutionary Cosmology . 10 1.3 Overview of the Dissertation . 22 I History of Cosmology 28 Chapter 2. The Origins of Early Universe Cosmology : : : : : : : : : : : : : : : : : 29 2.1 Development of the Standard Model . 33 2.1.1 Relativisitic Cosmology . 35 2.1.2 Thermal History . 40 2.2 Fine-Tuning Problems of the Standard Model . 45 2.2.1 Misner’s Chaotic Cosmology . 47 2.2.2 Particle Creation . 53 2.2.3 Baryogenesis . 57 2.3 The Horizon Problem . 60 2.4 Conclusions . 68 Chapter 3. False Vacuum : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 70 3.1 Eliminating the Singularity . 73 3.1.1 Λ in the USSR . 73 3.1.2 Starobinsky’s Model . 80 3.2 Hidden Symmetry . 85 3.2.1 Spontaneous Symmetry Breaking and the Higgs Mechanism . 86 3.2.2 Conformal Symmetry Breaking . 97 3.2.3 Symmetry Restoration . 101 3.3 Early Universe Phase Transitions . 106 3.4 Conclusions . 114 Chapter 4. An Inflationary Field : : : : : : : : : : : : : : : : : : : : : : : : : : : : 117 4.1 Old and New Inflation . 117 4.2 The Nuffield Workshop: Birth of the Inflaton . 131 4.3 The Baroque Era . 141 v II Philosophy of Cosmology 145 Chapter 5. Cosmological Principles : : : : : : : : : : : : : : : : : : : : : : : : : : 146 5.1 Two Approaches to Cosmology . 148 5.2 Global Aspects of Cosmology . 156 5.3 The Cosmological Principle . 163 5.3.1 Underdetermination . 163 5.3.2 Status of the CP . 177 5.4 The Indifference Principle . 179 5.4.1 Probabilities . 189 5.5 Anthropic Principles . 193 Chapter 6. Explanations in Cosmology : : : : : : : : : : : : : : : : : : : : : : : : 200 6.1 Unification . 202 6.1.1 Kitcher’s Account of Unification . 209 6.1.2 Unification in Cosmology . 216 6.2 Robustness and Causality . 224 6.2.1 Reichenbach’s Principle of the Common Cause . 226 6.2.2 Causality in the Early Universe . 233 6.2.3 Robustness . 239 6.3 Conclusion . 242 Chapter 7. Confirming Inflation : : : : : : : : : : : : : : : : : : : : : : : : : : : : 244 7.1 Testing Inflation I . 248 7.2 Testing Inflation II: Structure Formation . 255 7.3 Use-Novelty and Independence . 258 7.4 Inflation and Independence . 267 7.5 Robustness Revisited . 268 Appendix A . Aspects of Relativistic Cosmology : : : : : : : : : : : : : : : : : : : : 271 A.1 A Primer on General Relativity . 271 A.2 FLRW models . 279 A.3 Horizons . 284 A.4 Causal Structure . 288 A.5 No-Hair Theorems . 291 A.6 Conservation Laws . 293 Appendix B . Topics in Quantum Field Theory : : : : : : : : : : : : : : : : : : : : : 297 B.1 Spontaneous Symmetry Breaking . 297 B.2 Vacuum Energy . 299 Bibliography : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 302 vi List of Figures 2.1 The horizon problem . 61 3.1 Higgs potential . 105 4.1 “Old inflation” potential . 144 4.2 “New inflation” potential . 144 5.1 de Sitter solution . 171 5.2 WOI counterparts . 172 5.3 Ellis et al. (1978)’s model . 173 6.1 Illustration of the LCI . 232 A.1 Null Cone and Causal Sets . 289 vii Acknowledgments Without the encouragement and support from many people I would not have completed this dissertation, and I am indebted to all of them. Several institutions supported different aspects of this research. A grant from the Na- tional Science Foundation (SES 0114760) made it possible to perform interviews with cosmol- ogists, and I learned an enormous amount from the interviewees: John Barrow, Andrei Linde, Jeremiah Ostriker, James Peebles, Martin Rees, William Saslaw, Paul Steinhardt, and Neil Turok. I would also like to thank Spencer Weart at the American Institute of Physics (AIP) for support- ing the interview project. The AIP sponsored an interview with Charles Misner, a visit to the AIP archives, and transcription of all the interviews. Patrick McCray and Spencer Weart both gave me helpful advice. The Slater Fellowship from the American Philosophical Society gave me the freedom to extend the project in various ways, and I am very grateful for the award. I am also grateful for the generous financial support in various guises that I have received from the Department of History and Philosophy of Science. My greatest intellectual debt is to the members of my committee: John Earman, Al Janis, John Norton, and Laura Ruetsche. The work of the two Johns has set high standards for scholarship in the history and philosophy of science, and their advice and encouragement has helped me to come closer to attaining that standard. Conversations with John Earman initially inspired this project, and I owe a clear debt to his work on modern cosmology. His insightful comments at various stages have helped me to avoid a number of misconceptions. I benefitted enormously from John Norton’s thoughtful responses and suggestions, and discussions with John invariably led me to a much clearer conception of the issues at hand. Al Janis read everything I handed him with much more care than I had any right to expect, and his detailed comments improved the dissertation considerably. Laura Ruetsche consistently pointed me towards fruitful intersections between technical issues and the broader philosophical literature. Finally, I learned a great deal from Rob Clifton in the early stages of this work. His tragic early death robbed the community of one of its most insightful and penetrating scholars, and I sorely missed the opportunity to benefit from his further guidance. Many people contributed to the productive and engaging atmosphere of HPS and helped me enjoy my stint in graduate school. I thank Bernard Goldstein, Peter Machamer, and Ted McGuire for inspiring and encouraging my interest in early modern science and philosophy. Several friends have helped me to maintain my sanity through graduate school, but I am particu- larly indebted to Zvi Biener, Chris Martin, Greg Morgan, Wendy Parker, Gualtiero Piccinini, and John Roberts. I would like to thank my family for always encouraging me to pursue whatever career interested me, even if it meant leaving the farm and taking up something as bizarre as philosophy of science. They have been a constant source of support throughout my long career as a student. Finally, my greatest debt is to my wife, Sarah Gallagher. She has contributed directly to this dissertation in many ways, including drawing the figures, giving me LATEX advice, and patiently answering my questions about astrophysics. But more importantly, our relationship has been a constant source of strength and inspiration throughout the last eight years. I look forward to continuing this intellectual adventure together with Sarah. viii Nature, we ®nd, even from our limited experience, possesses an in®nite number of springs and prin- ciples, which incessantly discover themselves on every change of her position and situation. And what new and unknown principles would actuate her in so new and unknown a situation as that of the formation of a universe, we cannot, without the utmost temerity, pretend to determine. David Hume Cosmologists are often in error, but never in doubt. Lev Landau 1 Chapter 1 Introduction
Recommended publications
  • 5-Dimensional Space-Periodic Solutions of the Static Vacuum Einstein Equations
    5-DIMENSIONAL SPACE-PERIODIC SOLUTIONS OF THE STATIC VACUUM EINSTEIN EQUATIONS MARCUS KHURI, GILBERT WEINSTEIN, AND SUMIO YAMADA Abstract. An affirmative answer is given to a conjecture of Myers concerning the existence of 5-dimensional regular static vacuum solutions that balance an infinite number of black holes, which have Kasner asymp- totics. A variety of examples are constructed, having different combinations of ring S1 × S2 and sphere S3 cross-sectional horizon topologies. Furthermore, we show the existence of 5-dimensional vacuum solitons with Kasner asymptotics. These are regular static space-periodic vacuum spacetimes devoid of black holes. Consequently, we also obtain new examples of complete Riemannian manifolds of nonnegative Ricci cur- vature in dimension 4, and zero Ricci curvature in dimension 5, having arbitrarily large as well as infinite second Betti number. 1. Introduction The Majumdar-Papapetrou solutions [14, 16] of the 4D Einstein-Maxwell equations show that gravi- tational attraction and electro-magnetic repulsion may be balanced in order to support multiple black holes in static equilibrium. In [15], Myers generalized these solutions to higher dimensions, and also showed that such balancing is also possible for vacuum black holes in 4 dimensions if an infinite number are aligned properly in a periodic fashion along an axis of symmetry; these 4-dimensional solutions were later rediscovered by Korotkin and Nicolai in [11]. Although the Myers-Korotkin-Nicolai solutions are not asymptotically flat, but rather asymptotically Kasner, they play an integral part in an extended version of static black hole uniqueness given by Peraza and Reiris [17]. It was conjectured in [15] that these vac- uum solutions could be generalized to higher dimensions, possibly with black holes of nontrivial topology.
    [Show full text]
  • Supergravity Pietro Giuseppe Frè Dipartimento Di Fisica Teorica University of Torino Torino, Italy
    Gravity, a Geometrical Course Pietro Giuseppe Frè Gravity, a Geometrical Course Volume 2: Black Holes, Cosmology and Introduction to Supergravity Pietro Giuseppe Frè Dipartimento di Fisica Teorica University of Torino Torino, Italy Additional material to this book can be downloaded from http://extras.springer.com. ISBN 978-94-007-5442-3 ISBN 978-94-007-5443-0 (eBook) DOI 10.1007/978-94-007-5443-0 Springer Dordrecht Heidelberg New York London Library of Congress Control Number: 2012950601 © Springer Science+Business Media Dordrecht 2013 This work is subject to copyright. All rights are reserved by the Publisher, whether the whole or part of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilms or in any other physical way, and transmission or information storage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed. Exempted from this legal reservation are brief excerpts in connection with reviews or scholarly analysis or material supplied specifically for the purpose of being entered and executed on a computer system, for exclusive use by the purchaser of the work. Duplication of this publication or parts thereof is permitted only under the provisions of the Copyright Law of the Publisher’s location, in its current version, and permission for use must always be obtained from Springer. Permissions for use may be obtained through RightsLink at the Copyright Clearance Center. Violations are liable to prosecution under the respective Copyright Law. The use of general descriptive names, registered names, trademarks, service marks, etc.
    [Show full text]
  • A Domain Wall Solution by Perturbation of the Kasner Spacetime
    A Domain Wall Solution by Perturbation of the Kasner Spacetime George Kotsopoulos 1906-373 Front St. West, Toronto, ON M5V 3R7 [email protected] and Charles C. Dyer Dept. of Physical and Environmental Sciences, University of Toronto Scarborough, and Dept. of Astronomy and Astrophysics, University of Toronto, Toronto, Canada [email protected] January 24, 2012 Received ; accepted arXiv:1201.5362v1 [gr-qc] 25 Jan 2012 –2– Abstract Plane symmetric perturbations are applied to an axially symmetric Kasner spacetime which leads to no momentum flow orthogonal to the planes of symme- try. This flow appears laminar and the structure can be interpreted as a domain wall. We further extend consideration to the class of Bianchi Type I spacetimes and obtain corresponding results. Subject headings: general relativity, Kasner metric, Bianchi Type I, domain wall, perturbation –3– 1. Finding New Solutions There are three principal exact solutions to the Einstein Field Equations (EFE) that are most relevant for the description of astrophysical phenomena. They are the Schwarzschild (internal and external), Kerr and Friedman-LeMaître-Robertson-Walker (FLRW) models. These solutions are all highly idealized and involve the introduction of simplifying assumptions such as symmetry. The technique we use which has led to a solution of the EFE involves the perturbation of an already symmetric solution (Wilson and Dyer 2007). Whereas standard perturbation techniques involve specifying the forms of the energy-momentum tensor to determine the form of the metric, we begin by defining a new metric with an applied perturbation: gab =g ˜ab + hab (1) where g˜ab is a known symmetric metric and hab is the applied perturbation.
    [Show full text]
  • Analog Geometry in an Expanding Fluid from Ads/CFT Perspective
    Physics Letters B 743 (2015) 340–346 Contents lists available at ScienceDirect Physics Letters B www.elsevier.com/locate/physletb Analog geometry in an expanding fluid from AdS/CFT perspective ∗ Neven Bilic´ , Silvije Domazet, Dijana Tolic´ Division of Theoretical Physics, Rudjer Boškovi´c Institute, P.O. Box 180, 10001 Zagreb, Croatia a r t i c l e i n f o a b s t r a c t Article history: The dynamics of an expanding hadron fluid at temperatures below the chiral transition is studied in Received 16 February 2015 the framework of AdS/CFT correspondence. We establish a correspondence between the asymptotic AdS Accepted 5 March 2015 geometry in the 4 + 1dimensional bulk with the analog spacetime geometry on its 3 + 1dimensional Available online 9 March 2015 boundary with the background fluid undergoing a spherical Bjorken type expansion. The analog metric Editor: L. Alvarez-Gaumé tensor on the boundary depends locally on the soft pion dispersion relation and the four-velocity of Keywords: the fluid. The AdS/CFT correspondence provides a relation between the pion velocity and the critical Analogue gravity temperature of the chiral phase transition. AdS/CFT correspondence © 2015 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license 3 Chiral phase transition (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP . Linear sigma model Bjorken expansion 1. Introduction found in the QCD vacuum and its non-vanishing value is a man- ifestation of chiral symmetry breaking [8]. The chiral symmetry The original formulation of gauge-gravity duality in the form of is restored at finite temperature through a chiral phase transition the so called AdS/CFT correspondence establishes an equivalence of which is believed to be of first or second order depending on the a four dimensional N = 4 supersymmetric Yang–Mills theory and underlying global symmetry [9].
    [Show full text]
  • Particle Production in the Central Rapidity Region
    LA-UR-92-3856 November, 1992 Particle production in the central rapidity region F. Cooper,1 J. M. Eisenberg,2 Y. Kluger,1;2 E. Mottola,1 and B. Svetitsky2 1Theoretical Division and Center for Nonlinear Studies Los Alamos National Laboratory Los Alamos, New Mexico 87545 USA 2School of Physics and Astronomy Raymond and Beverly Sackler Faculty of Exact Sciences Tel Aviv University, 69978 Tel Aviv, Israel ABSTRACT We study pair production from a strong electric ¯eld in boost- invariant coordinates as a simple model for the central rapidity region of a heavy-ion collision. We derive and solve the renormal- ized equations for the time evolution of the mean electric ¯eld and current of the produced particles, when the ¯eld is taken to be a function only of the fluid proper time ¿ = pt2 z2. We ¯nd that a relativistic transport theory with a Schwinger¡source term mod- i¯ed to take Pauli blocking (or Bose enhancement) into account gives a good description of the numerical solution to the ¯eld equations. We also compute the renormalized energy-momentum tensor of the produced particles and compare the e®ective pres- sure, energy and entropy density to that expected from hydrody- namic models of energy and momentum flow of the plasma. 1 Introduction A popular theoretical picture of high-energy heavy-ion collisions begins with the creation of a flux tube containing a strong color electric ¯eld [1]. The ¯eld energy is converted into particles as qq¹ pairs and gluons are created by the Schwinger tunneling mechanism [2, 3, 4]. The transition from this quantum tunneling stage to a later hydrodynamic stage has previously been described phenomenologically using a kinetic theory model in which a rel- ativistic Boltzmann equation is coupled to a simple Schwinger source term [5, 6, 7, 8].
    [Show full text]
  • On Limiting Curvature in Mimetic Gravity
    On limiting curvature in mimetic gravity Tobias Benjamin Russ München 2021 On limiting curvature in mimetic gravity Tobias Benjamin Russ Dissertation an der Fakultät für Physik der Ludwig–Maximilians–Universität München vorgelegt von Tobias Benjamin Russ aus Güssing, Österreich München, den 11. Mai 2021 Erstgutachter: Prof. Dr. Viatcheslav Mukhanov, LMU München Zweitgutachter: Prof. Dr. Paul Steinhardt, Princeton University Tag der mündlichen Prüfung: 8. Juli 2021 Contents Zusammenfassung . vii Abstract . ix Acknowledgements . xi Publications . xiii Summary 1 0.1 Introduction . .1 0.2 The theory . .7 0.3 Results & Conclusions . 12 0.3.1 Big Bang replaced by initial dS . 12 0.3.2 Anisotropic singularity resolution requires asymptotic freedom . 17 0.3.3 Modified black hole with stable remnant . 20 0.3.4 Higher spatial derivatives avert gradient instability . 26 0.4 Outlook . 30 1 Asymptotically Free Mimetic Gravity 31 1.1 Introduction . 32 1.2 Action and equations of motion . 33 1.3 The synchronous coordinate system . 33 1.4 Asymptotic freedom and the fate of a collapsing universe . 35 1.5 Quantum fluctuations . 39 1.6 Conclusions . 40 2 Mimetic Hořava Gravity 43 3 Black Hole Remnants 49 3.1 Introduction . 50 3.2 The Lemaître coordinates . 50 3.3 Modified Mimetic Gravity . 51 3.4 Asymptotic Freedom at Limiting Curvature . 52 3.5 Exact Solution . 53 3.6 Black hole thermodynamics . 55 3.7 Conclusions . 56 vi Contents 4 Non-flat Universes and Black Holes in A.F.M.G. 57 4.1 The Theory . 58 4.1.1 Introduction . 58 4.1.2 Action and equations of motion .
    [Show full text]
  • Symbols 1-Form, 10 4-Acceleration, 184 4-Force, 115 4-Momentum, 116
    Index Symbols B 1-form, 10 Betti number, 589 4-acceleration, 184 Bianchi type-I models, 448 4-force, 115 Bianchi’s differential identities, 60 4-momentum, 116 complex valued, 532–533 total, 122 consequences of in Newman-Penrose 4-velocity, 114 formalism, 549–551 first contracted, 63 second contracted, 63 A bicharacteristic curves, 620 acceleration big crunch, 441 4-acceleration, 184 big-bang cosmological model, 438, 449 Newtonian, 74 Birkhoff’s theorem, 271 action function or functional bivector space, 486 (see also Lagrangian), 594, 598 black hole, 364–433 ADM action, 606 Bondi-Metzner-Sachs group, 240 affine parameter, 77, 79 boost, 110 alternating operation, antisymmetriza- Born-Infeld (or tachyonic) scalar field, tion, 27 467–471 angle field, 44 Boyer-Lindquist coordinate chart, 334, anisotropic fluid, 218–220, 276 399 collapse, 424–431 Brinkman-Robinson-Trautman met- ric, 514 anti-de Sitter space-time, 195, 644, Buchdahl inequality, 262 663–664 bugle, 69 anti-self-dual, 671 antisymmetric oriented tensor, 49 C antisymmetric tensor, 28 canonical energy-momentum-stress ten- antisymmetrization, 27 sor, 119 arc length parameter, 81 canonical or normal forms, 510 arc separation function, 85 Cartesian chart, 44, 68 arc separation parameter, 77 Casimir effect, 638 Arnowitt-Deser-Misner action integral, Cauchy horizon, 403, 416 606 Cauchy problem, 207 atlas, 3 Cauchy-Kowalewski theorem, 207 complete, 3 causal cone, 108 maximal, 3 causal space-time, 663 698 Index 699 causality violation, 663 contravariant index, 51 characteristic hypersurface, 623 contravariant
    [Show full text]
  • Arxiv:2008.13699V3 [Hep-Th] 18 Mar 2021 1 Rsn Drs:Dprmn Fpyis Ea Ae Olg,S College, Patel Vesaj Physics, of Department Address: Present Xadn Udi H Aetm Regime
    Anisotropic expansion, second order hydrodynamics and holographic dual Priyanka Priyadarshini Pruseth 1 and Swapna Mahapatra Department of Physics, Utkal University, Bhubaneswar 751004, India. [email protected] , [email protected] Abstract We consider Kasner space-time describing anisotropic three dimensional expan- sion of RHIC and LHC fireball and study the generalization of Bjorken’s one dimensional expansion by taking into account second order relativistic viscous hydrodynamics. Using time dependent AdS/CFT correspondence, we study the late time behaviour of the Bjorken flow. From the conditions of conformal invariance and energy-momentum conservation, we obtain the explicit expres- sion for the energy density as a function of proper time in terms of Kasner parameters. The proper time dependence of the temperature and entropy have also been obtained in terms of Kasner parameters. We consider Eddington- Finkelstein type coordinates and discuss the gravity dual of the anisotropically expanding fluid in the late time regime. arXiv:2008.13699v3 [hep-th] 18 Mar 2021 1Present address: Department of Physics, Vesaj Patel College, Sundargarh, India 1 Introduction AdS/CFT correspondence has provided a very important tool for studying the strongly coupled dynamics in a class of superconformal field theories, in particular, = 4 super N Yang-Mills theory and the corresponding gravity dual description in AdS space-time [1, 2]. One of the fundamental question in the field of high energy physics is to understand the properties of matter at extreme density and temperature in the first few microseconds after the big bang. Such a state of matter is known as Quark-Gluon-Plasma (QGP) state where the quarks and the gluons are in deconfined state.
    [Show full text]
  • "Behaviour of the Gravitational Field Around the Initial Singularity"
    "BEHAVIOUR OF THE GRAVITATIONAL FIELD AROUND THE INITIAL SINGULARITY" Gerson Francisco. t ? õ INSTIT0T0 01 flSICA TEÓRICA "BEHAVIOUR OF THE GRAVITATIONAL FIELD AROUND THE INITIAL SINGULARITY" Gerson Francisco Instituto de Física Teórica Rua Pamplona, 145 01405 - São Paulo-SP BRASIL. Abstract The ultralocal representation of the canonical^ ly quantized gravitational field is used to obtain the evolution of coherent states in the immediate neighborhood of the singulari- ty. It is shown that smearing functions play the role of classical fields since they correspond to cosrnological solutions around the singularity. A special class of ultralocal coherent states is shown to contain the essential aspects of the dynamics of the system when we choose a simple representation for the field operators of the theory. When the ultralocality condition is broken a conjec- ture will be made about the quantum evolution of coherent states in the classical limit. i-í . Intiüd^': I ion Cosmologica.1 solutions to Einstein equations a-o'jnd the Initial singularity have been thouroughly investigated _y b^Lin^kii, KhaiaLnikov and Lifshitz |1—3| (or BKL t\u short). [n fiLs connection ue also mention the u»ork of Eardley et al. |4| inn thu Hami ltoninr' tiaatment of Liang |5|. The main point of theso st'ciRs is ttip far:t thac a large class of solutions to Einstein rtn,iaf,ions \n r.ne asymptotic region close to the singularity exhi- ;•>: ' :. kifnj cr ?\.>antaneously decoupled dynamics in the sense that field ewoJution at a given initial point on a Cauchy hypersur- 5^ is totally independent from what occurs in its neighbor- hood.
    [Show full text]
  • University of California Santa Cruz a Model of Spacetime
    UNIVERSITY OF CALIFORNIA SANTA CRUZ A MODEL OF SPACETIME EMERGENCE IN THE EARLY UNIVERSE A dissertation submitted in partial satisfaction of the requirements for the degree of DOCTOR OF PHILOSOPHY in PHYSICS by Martin W. Tysanner September 2012 The Dissertation of Martin W. Tysanner is approved: Anthony Aguirre, Chair Michael Dine Stefano Profumo Tyrus Miller Vice Provost and Dean of Graduate Studies Copyright c by Martin W. Tysanner 2012 Table of Contents Abstract vi Dedication viii Acknowledgments ix 1 Introduction 1 1.1 Aims and overview . .1 1.2 Inflation and its difficulties . .2 1.2.1 Penrose's entropy argument . .3 1.2.2 Predictivity problem of eternal inflation . .5 1.3 Assessment . .8 1.3.1 Motivation for an emergence picture . 10 1.4 Overview of the Emergence Picture . 12 1.5 Thesis Plan . 19 1.5.1 Thesis outline . 19 1.5.2 How to read this thesis . 22 1.6 Notation and Conventions . 23 I Pre-Emergent Space 28 2 Foundation 29 2.1 Topological Space (Σ; TΣ).......................... 31 2.2 Irreducible Field ' on (Σ; d)......................... 40 2.2.1 Elementary oscillator field,! ~[M].................. 41 2.2.2 Intrinsic stochasticity of ' ...................... 44 2.2.3 Elementary dynamics of ' ...................... 47 2.2.4 Preferred scale . 56 3 Stochastic Processes and Calculus of ' 58 3.1 Stochastic Processes . 59 3.1.1 Stochastic processes and Brownian motion . 59 3.1.2 Spectral analysis of stochastic functions . 66 3.2 Stochastic Calculus . 72 iii 3.2.1 Stochastic differentials . 72 3.2.2 Stochastic integrals . 73 3.3 Differentiation of ' .............................
    [Show full text]
  • The Wave Equation Near Flat Friedmann–Lemaître–Robertson–Walker and Kasner Big Bang Singularities Artur Alho, Grigorios Fournodavlos, Anne Franzen
    The wave equation near flat Friedmann–Lemaître–Robertson–Walker and Kasner Big Bang singularities Artur Alho, Grigorios Fournodavlos, Anne Franzen To cite this version: Artur Alho, Grigorios Fournodavlos, Anne Franzen. The wave equation near flat Friedmann–Lemaître– Robertson–Walker and Kasner Big Bang singularities. Journal of Hyperbolic Differential Equations, World Scientific Publishing, 2019, 16 (02), pp.379-400. 10.1142/S0219891619500140. hal-02967520 HAL Id: hal-02967520 https://hal.sorbonne-universite.fr/hal-02967520 Submitted on 15 Oct 2020 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. THE WAVE EQUATION NEAR FLAT FRIEDMANN-LEMA^ITRE-ROBERTSON-WALKER AND KASNER BIG BANG SINGULARITIES Artur Alho1;?, Grigorios Fournodavlos2;y, and Anne T. Franzen3;? ?Center for Mathematical Analysis, Geometry and Dynamical Systems, Instituto Superior T´ecnico, Universidade de Lisboa, Av. Rovisco Pais, 1049-001 Lisboa, Portugal y Department of Pure Mathematics and Mathematical Statistics, University of Cambridge, Wilberforce Road, Cambridge CB3 0WB, United Kingdom Abstract. We consider the wave equation, g = 0, in fixed flat Friedmann-Lema^ıtre-Robertson-Walker 3 and Kasner spacetimes with topology R+ × T . We obtain generic blow up results for solutions to the wave equation towards the Big Bang singularity in both backgrounds.
    [Show full text]
  • Kasner Branes with Arbitrary Signature
    Physics Letters B 809 (2020) 135694 Contents lists available at ScienceDirect Physics Letters B www.elsevier.com/locate/physletb Kasner branes with arbitrary signature W.A. Sabra Department of Physics, American University of Beirut, Lebanon a r t i c l e i n f o a b s t r a c t Article history: We present static and time-dependent solutions for the theory of gravity with a dilaton field and Received 22 July 2020 an arbitrary rank antisymmetric tensor. The solutions constructed are valid for arbitrary space-time Received in revised form 4 August 2020 dimensions and signatures. Accepted 7 August 2020 © 2020 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license Available online 13 August 2020 (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP3. Editor: N. Lambert 1. Introduction Many years ago, Kasner [1]presented Euclidean four-dimensional vacuum solutions which depend only on one variable. Those solutions can be written in the form 2 = 2a1 2 + 2a2 2 + 2a3 2 + 2a4 2 ds x1 dx1 x1 dx2 x1 dx3 x1 dx4, (1.1) where the constants appearing in the metric, the Kasner exponents, satisfy the following conditions a2 + a3 + a4 = 1 + a1, 2 + 2 + 2 = + 2 a2 a3 a4 (1 a1) . (1.2) The Kasner metric is actually valid for all space-time signatures [2]. If one writes 2 = 2a1 2 + 2a2 2 + 2a3 2 + 2a4 2 ds 0x1 dx1 1x1 dx2 2x1 dx3 3x1 dx4, (1.3) where i takes the values ±1, then the metric (1.3)can be shown to be a vacuum solution for four-dimensional gravity with all possible space-time signatures provided the Kasner conditions (1.2)are satisfied.
    [Show full text]