Spectral Approach to the Axisymmetric Evolution of Einstein's Vacuum
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General Relativity As Taught in 1979, 1983 By
General Relativity As taught in 1979, 1983 by Joel A. Shapiro November 19, 2015 2. Last Latexed: November 19, 2015 at 11:03 Joel A. Shapiro c Joel A. Shapiro, 1979, 2012 Contents 0.1 Introduction............................ 4 0.2 SpecialRelativity ......................... 7 0.3 Electromagnetism. 13 0.4 Stress-EnergyTensor . 18 0.5 Equivalence Principle . 23 0.6 Manifolds ............................. 28 0.7 IntegrationofForms . 41 0.8 Vierbeins,Connections . 44 0.9 ParallelTransport. 50 0.10 ElectromagnetisminFlatSpace . 56 0.11 GeodesicDeviation . 61 0.12 EquationsDeterminingGeometry . 67 0.13 Deriving the Gravitational Field Equations . .. 68 0.14 HarmonicCoordinates . 71 0.14.1 ThelinearizedTheory . 71 0.15 TheBendingofLight. 77 0.16 PerfectFluids ........................... 84 0.17 Particle Orbits in Schwarzschild Metric . 88 0.18 AnIsotropicUniverse. 93 0.19 MoreontheSchwarzschild Geometry . 102 0.20 BlackHoleswithChargeandSpin. 110 0.21 Equivalence Principle, Fermions, and Fancy Formalism . .115 0.22 QuantizedFieldTheory . .121 3 4. Last Latexed: November 19, 2015 at 11:03 Joel A. Shapiro Note: This is being typed piecemeal in 2012 from handwritten notes in a red looseleaf marked 617 (1983) but may have originated in 1979 0.1 Introduction I am, myself, an elementary particle physicist, and my interest in general relativity has come from the growth of a field of quantum gravity. Because the gravitational inderactions of reasonably small objects are so weak, quantum gravity is a field almost entirely divorced from contact with reality in the form of direct confrontation with experiment. There are three areas of contact 1. In relativistic quantum mechanics, one usually formulates the physical quantities in terms of fields. A field is a physical degree of freedom, or variable, definded at each point of space and time. -
3+1 Formalism and Bases of Numerical Relativity
3+1 Formalism and Bases of Numerical Relativity Lecture notes Eric´ Gourgoulhon Laboratoire Univers et Th´eories, UMR 8102 du C.N.R.S., Observatoire de Paris, Universit´eParis 7 arXiv:gr-qc/0703035v1 6 Mar 2007 F-92195 Meudon Cedex, France [email protected] 6 March 2007 2 Contents 1 Introduction 11 2 Geometry of hypersurfaces 15 2.1 Introduction.................................... 15 2.2 Frameworkandnotations . .... 15 2.2.1 Spacetimeandtensorfields . 15 2.2.2 Scalar products and metric duality . ...... 16 2.2.3 Curvaturetensor ............................... 18 2.3 Hypersurfaceembeddedinspacetime . ........ 19 2.3.1 Definition .................................... 19 2.3.2 Normalvector ................................. 21 2.3.3 Intrinsiccurvature . 22 2.3.4 Extrinsiccurvature. 23 2.3.5 Examples: surfaces embedded in the Euclidean space R3 .......... 24 2.4 Spacelikehypersurface . ...... 28 2.4.1 Theorthogonalprojector . 29 2.4.2 Relation between K and n ......................... 31 ∇ 2.4.3 Links between the and D connections. .. .. .. .. .. 32 ∇ 2.5 Gauss-Codazzirelations . ...... 34 2.5.1 Gaussrelation ................................. 34 2.5.2 Codazzirelation ............................... 36 3 Geometry of foliations 39 3.1 Introduction.................................... 39 3.2 Globally hyperbolic spacetimes and foliations . ............. 39 3.2.1 Globally hyperbolic spacetimes . ...... 39 3.2.2 Definition of a foliation . 40 3.3 Foliationkinematics .. .. .. .. .. .. .. .. ..... 41 3.3.1 Lapsefunction ................................. 41 3.3.2 Normal evolution vector . 42 3.3.3 Eulerianobservers ............................. 42 3.3.4 Gradients of n and m ............................. 44 3.3.5 Evolution of the 3-metric . 45 4 CONTENTS 3.3.6 Evolution of the orthogonal projector . ....... 46 3.4 Last part of the 3+1 decomposition of the Riemann tensor . -
Part 3 Black Holes
Part 3 Black Holes Harvey Reall Part 3 Black Holes March 13, 2015 ii H.S. Reall Contents Preface vii 1 Spherical stars 1 1.1 Cold stars . .1 1.2 Spherical symmetry . .2 1.3 Time-independence . .3 1.4 Static, spherically symmetric, spacetimes . .4 1.5 Tolman-Oppenheimer-Volkoff equations . .5 1.6 Outside the star: the Schwarzschild solution . .6 1.7 The interior solution . .7 1.8 Maximum mass of a cold star . .8 2 The Schwarzschild black hole 11 2.1 Birkhoff's theorem . 11 2.2 Gravitational redshift . 12 2.3 Geodesics of the Schwarzschild solution . 13 2.4 Eddington-Finkelstein coordinates . 14 2.5 Finkelstein diagram . 17 2.6 Gravitational collapse . 18 2.7 Black hole region . 19 2.8 Detecting black holes . 21 2.9 Orbits around a black hole . 22 2.10 White holes . 24 2.11 The Kruskal extension . 25 2.12 Einstein-Rosen bridge . 28 2.13 Extendibility . 29 2.14 Singularities . 29 3 The initial value problem 33 3.1 Predictability . 33 3.2 The initial value problem in GR . 35 iii CONTENTS 3.3 Asymptotically flat initial data . 38 3.4 Strong cosmic censorship . 38 4 The singularity theorem 41 4.1 Null hypersurfaces . 41 4.2 Geodesic deviation . 43 4.3 Geodesic congruences . 44 4.4 Null geodesic congruences . 45 4.5 Expansion, rotation and shear . 46 4.6 Expansion and shear of a null hypersurface . 47 4.7 Trapped surfaces . 48 4.8 Raychaudhuri's equation . 50 4.9 Energy conditions . 51 4.10 Conjugate points . -
HARMONIC MORPHISMS BETWEEN RIEMANNIAN MANIFOLDS by Bent FUGLEDE
Ann. Inst. Fourier, Grenoble 28, 2 (1978), 107-144, HARMONIC MORPHISMS BETWEEN RIEMANNIAN MANIFOLDS by Bent FUGLEDE Introduction. The harmonic morphisms of a Riemannian manifold, M , into another, N , are the morphisms for the harmonic struc- tures on M and N (the harmonic functions on a Riemannian manifold being those which satisfy the Laplace-Beltrami equation). These morphisms were introduced and studied by Constantinescu and Cornea [4] in the more general frame of harmonic spaces, as a natural generalization of the conformal mappings between Riemann surfaces (1). See also Sibony [14]. The present paper deals with harmonic morphisms between two Riemannian manifolds M and N of arbitrary (not necessarily equal) dimensions. It turns out, however, that if dim M < dim N , the only harmonic morphisms M -> N are the constant mappings. Thus we are left with the case dim M ^ dim N . If dim N = 1 , say N = R , the harmonic morphisms M —> R are nothing but the harmonic functions on M . If dim M = dim N = 2 , so that M and N are Riemann surfaces, then it is known that the harmonic morphisms of (1) We use the term « harmonic morphisms » rather than « harmonic maps » (as they were called in the case of harmonic spaces in [4]) since it is necessary (in the present frame of manifolds) to distinguish between these maps and the much wider class of harmonic maps in the sense of Eells and Sampson [7], which also plays an important role in our discussion. 108 B. FUGLEDE M into N are the same as the conformal mappings f: M -> N (allowing for points where df= 0). -
Partial Differential Equations
PARTIAL DIFFERENTIAL EQUATIONS SERGIU KLAINERMAN 1. Basic definitions and examples To start with partial differential equations, just like ordinary differential or integral equations, are functional equations. That means that the unknown, or unknowns, we are trying to determine are functions. In the case of partial differential equa- tions (PDE) these functions are to be determined from equations which involve, in addition to the usual operations of addition and multiplication, partial derivatives of the functions. The simplest example, which has already been described in section 1 of this compendium, is the Laplace equation in R3, ∆u = 0 (1) ∂2 ∂2 ∂2 where ∆u = ∂x2 u + ∂y2 u + ∂z2 u. The other two examples described in the section of fundamental mathematical definitions are the heat equation, with k = 1, − ∂tu + ∆u = 0, (2) and the wave equation with k = 1, 2 − ∂t u + ∆u = 0. (3) In these last two cases one is asked to find a function u, depending on the variables t, x, y, z, which verifies the corresponding equations. Observe that both (2) and (3) involve the symbol ∆ which has the same meaning as in the first equation, that is ∂2 ∂2 ∂2 ∂2 ∂2 ∂2 ∆u = ( ∂x2 + ∂y2 + ∂z2 )u = ∂x2 u+ ∂y2 u+ ∂z2 u. Both equations are called evolution equations, simply because they are supposed to describe the change relative to the time parameter t of a particular physical object. Observe that (1) can be interpreted as a particular case of both (3) and (2). Indeed solutions u = u(t, x, y, z) of either (3) or (2) which are independent of t, i.e. -
Riemannian Geometry
Appendix A Riemannian Geometry In this appendix besides introducing notation and basic definitions we recollect some of the more technical results in Riemannian geometry we exploited in these lecture notes. We freely refer to the excellent exposition of the theory provided by [4, 8], and to [27] for further details. A.1 Notation In what follows, Vn will always denote a C1 compact n–dimensional manifold, (n 3). Unless otherwise stated, the manifold Vn will be supposed oriented, connected, and without boundary. Let .E; Vn;/be a smooth vector bundle over Vn with projection map W E ! Vn. When no confusion arises the space of smooth 1. n; / n 1. n; / sections fs 2 C V E j ı s D idV g will simply be denoted by C V E instead of the standard .E/ (to avoid confusion (Fig. A.1) with the already too numerous s appearing in Riemannian geometry: Christoffel symbols, harmonic n i n coordinates, ...).If U V is an open set, we let fx giD1 be local coordinates for @ @=@ i n 1. ; n/ the points p 2 U. The vector fields f i WD x giD1 2 C U TV provide the n local (positively oriented) coordinate basis for TpV , p 2 U. The corresponding n 1 dual basis for the cotangent spaces Tp V , is provided by the set of –forms i n 1. ; n/ 1. n; 2 n/ fdx giD1 2 C U T V . In particular, the metric tensor g 2 C V ˝S T V , 1. n; 2 n/ where C V ˝S T V denotes the set of smooth symmetric bilinear forms over n i k V , has the local coordinates representation g D gikdx ˝dx , where gik WD g.@i;@k/, and the Einsteinp summation convention is in effect. -
Catalogue of Spacetimes
Catalogue of Spacetimes e2 e1 x2 = 2 x = 2 q ∂x2 1 x2 = 1 ∂x1 x1 = 1 x1 = 0 x2 = 0 M Authors: Thomas Müller Visualisierungsinstitut der Universität Stuttgart (VISUS) Allmandring 19, 70569 Stuttgart, Germany [email protected] Frank Grave formerly, Universität Stuttgart, Institut für Theoretische Physik 1 (ITP1) Pfaffenwaldring 57 //IV, 70550 Stuttgart, Germany [email protected] URL: http://go.visus.uni-stuttgart.de/CoS Date: 21. Mai 2014 Co-authors Andreas Lemmer, formerly, Institut für Theoretische Physik 1 (ITP1), Universität Stuttgart Alcubierre Warp Sebastian Boblest, Institut für Theoretische Physik 1 (ITP1), Universität Stuttgart deSitter, Friedmann-Robertson-Walker Felix Beslmeisl, Institut für Theoretische Physik 1 (ITP1), Universität Stuttgart Petrov-Type D Heiko Munz, Institut für Theoretische Physik 1 (ITP1), Universität Stuttgart Bessel and plane wave Andreas Wünsch, Institut für Theoretische Physik 1 (ITP1), Universität Stuttgart Majumdar-Papapetrou, extreme Reissner-Nordstrøm dihole, energy momentum tensor Many thanks to all that have reported bug fixes or added metric descriptions. Contents 1 Introduction and Notation1 1.1 Notation...............................................1 1.2 General remarks...........................................1 1.3 Basic objects of a metric......................................2 1.4 Natural local tetrad and initial conditions for geodesics....................3 1.4.1 Orthonormality condition.................................3 1.4.2 Tetrad transformations...................................4 -
An Introduction to the Theory of Rotating Relativistic Stars
An introduction to the theory of rotating relativistic stars Lectures at the COMPSTAR 2010 School GANIL, Caen, France, 8-16 February 2010 Éric Gourgoulhon Laboratoire Univers et Théories, UMR 8102 du CNRS, Observatoire de Paris, Université Paris Diderot - Paris 7 92190 Meudon, France [email protected] arXiv:1003.5015v2 [gr-qc] 20 Sep 2011 20 September 2011 2 Contents Preface 5 1 General relativity in brief 7 1.1 Geometrical framework . ..... 7 1.1.1 The spacetime of general relativity . ....... 7 1.1.2 Linearforms .................................. 9 1.1.3 Tensors ..................................... 10 1.1.4 Metrictensor .................................. 10 1.1.5 Covariant derivative . 11 1.2 Einsteinequation................................ .... 13 1.3 3+1formalism .................................... 14 1.3.1 Foliation of spacetime . 15 1.3.2 Eulerian observer or ZAMO . 16 1.3.3 Adapted coordinates and shift vector . ....... 17 1.3.4 Extrinsic curvature . 18 1.3.5 3+1 Einstein equations . 18 2 Stationary and axisymmetric spacetimes 21 2.1 Stationary and axisymmetric spacetimes . .......... 21 2.1.1 Definitions ................................... 21 2.1.2 Stationarity and axisymmetry . ..... 25 2.2 Circular stationary and axisymmetric spacetimes . ............. 27 2.2.1 Orthogonal transitivity . ..... 27 2.2.2 Quasi-isotropic coordinates . ...... 29 2.2.3 Link with the 3+1 formalism . 31 3 Einstein equations for rotating stars 33 3.1 Generalframework ................................ 33 3.2 Einstein equations in QI coordinates . ......... 34 3.2.1 Derivation.................................... 34 3.2.2 Boundary conditions . 36 3.2.3 Caseofaperfectfluid ............................ 37 3.2.4 Newtonianlimit ................................ 39 3.2.5 Historicalnote ................................ 39 3.3 Spherical symmetry limit . ..... 40 3.3.1 Takingthelimit ............................... -
Applications of Partial Differential Equations to Problems in Geometry
Applications of Partial Differential Equations To Problems in Geometry Jerry L. Kazdan Preliminary revised version Copyright c 1983, 1993 by Jerry L. Kazdan ° Preface These notes are from an intensive one week series of twenty lectures given to a mixed audience of advanced graduate students and more experienced mathematicians in Japan in July, 1983. As a consequence, these they are not aimed at experts, and are frequently quite detailed, especially in Chapter 6 where a variety of standard techniques are presented. My goal was to in- troduce geometers to some of the techniques of partial differential equations, and to introduce those working in partial differential equations to some fas- cinating applications containing many unresolved nonlinear problems arising in geometry. My intention is that after reading these notes someone will feel that they can cope with current research articles. In fact, the quite sketchy Chapter 5 and Chapter 6 are merely intended to be advertisements to read the complete details in the literature. When writing something like this, there is the very real danger that the only people who understand anything are those who already know the subject. Caveat emptor. In any case, I hope I have shown that if one assumes a few basic results on Sobolev spaces and elliptic operators, then the basic techniques used in the applications are comprehensible. Of course carrying out the details for any specific problem may be quite complicated—but at least the ideas should be clearly recognizable. These notes definitely do not represent the whole subject. I did not have time to discuss a number of beautiful applications such as minimal surfaces, harmonic maps, global isometric embeddings (including the Weyl and Minkowski problems as well as Nash’s theorem), Yang-Mills fields, the wave equation and spectrum of the Laplacian, and problems on compact manifolds with boundary or complete non-compact manifolds. -
Boundary Behavior of Harmonic Maps on Non-Smooth Domains and Complete Negatively Curved Manifolds*
JOURNAL OF FUNCTIONAL ANALYSIS 99, 293-33 1 (1991) Boundary Behavior of Harmonic Maps on Non-smooth Domains and Complete Negatively Curved Manifolds* PATRICTO Avrr.ks Deporrmenl oj Muthrmarics, University of Illinms at Urbana-Champaign, Urbana. Illinois 61801 H. CHOI Department oJ Mathematics, University qf‘ Iouaa. Iowa City, Iowa 52242 AND MARIO MICALLEF Department of Mathematics, University of Warwick, Convenrry CV4 7AL, England. Communicated by R. B. Melrose Received November 8, 1989 In this paper we develop a theory for harmonic maps which is analogous to the classical theory for bounded harmonic functions in harmonic analysis. We solve the Dirichlet problem in bounded Lipschitz domains and manifolds with negative sectional curvatures, generalize the Wienner criterion, and prove the Fatou theorem for harmonic maps into convex balls. Ii” 1991 Academic Press. Inc. CONTENTS 1. Introduction and statement of main results. 2. Preliminaries and notation. 3. The Dirichlet problem in regular domains and Wiener criterion for harmonic maps. 4. The Dirichlet problem on complete, negatively curved manifolds. 5. Fatou’s theorem for harmonic maps into convex balls. 6. Bounded Lipschitz domains in complete Riemannian manifolds. * All of the authors were supported by NSF grants. 293 0022-1236191$3.00 Copyright % 1991 by Academx Press, Inc All rlghfs of reproductmn m any form reserved 294 AWL&, CHOI, AND MICALLEF 1. INTRODUCTION AND STATEMENT OF RESULTS The Dirichlet problem and Fatou’s theorem are central topics of investigation in harmonic analysis on bounded domains. The main point of this paper is to extend such properties of harmonic functions to harmonic maps whose image lies in a convex ball. -
Cheeger-Gromov Theory and Applications to General Relativity
CHEEGER-GROMOV THEORY AND APPLICATIONS TO GENERAL RELATIVITY MICHAEL T. ANDERSON Contents 1. Background: Examples and Definitions. 1 2. Convergence/Compactness. 5 3. Collapse/Formation of Cusps. 11 4. Applications to Static and Stationary Space-Times. 16 5. Lorentzian Analogues and Open Problems. 21 6. Future Asymptotics and Geometrization of 3-Manifolds. 27 References 30 This paper surveys aspects of the convergence and degeneration of Rie- mannian metrics on a given manifold M, and some recent applications of this theory to general relativity. The basic point of view of conver- gence/degeneration described here originates in the work of Gromov, cf. [31]-[33], with important prior work of Cheeger [16], leading to the joint work of [18]. This Cheeger-Gromov theory assumes L∞ bounds on the full curvature tensor. For reasons discussed below, we focus mainly on the generalizations ∞ p arXiv:gr-qc/0208079v2 28 Jan 2004 of this theory to spaces with L , (or L ) bounds on the Ricci curvature. Although versions of the results described hold in any dimension, for the most part we restrict the discussion to 3 and 4 dimensions, where stronger results hold and the applications to general relativity are most direct. The first three sections survey the theory in Riemannian geometry, while the last three sections discuss applications to general relativity. I am grateful to many of the participants of the Carg`ese meeting for their comments and suggestions, and in particular to Piotr Chru´sciel and Helmut Friedrich for organizing such a fine meeting. 1. Background: Examples and Definitions. The space M of Riemannian metrics on a given manifold M is an infinite dimensional cone, (in the vector space of symmetric bilinear forms on M), Partially supported by NSF Grant DMS 0072591. -
Version1326.1.K
Contents 26 Relativistic Stars and Black Holes 1 26.1Overview...................................... 1 26.2 Schwarzschild’s Spacetime Geometry . ....... 2 26.2.1 The Schwarzschild Metric, its Connection Coefficients, and its Curva- tureTensors................................ 2 26.2.2 The Nature of Schwarzschild’s Coordinate System, and Symmetries of the Schwarzschild Spacetime . 4 26.2.3 Schwarzschild Spacetime at Radii r ≫ M: The Asymptotically Flat Region................................... 5 26.2.4 Schwarzschild Spacetime at r ∼ M ................... 7 26.3StaticStars .................................... 9 26.3.1 Birkhoff’sTheorem ............................ 9 26.3.2 StellarInterior .............................. 11 26.3.3 Local Conservation of Energy and Momentum . .... 14 26.3.4 EinsteinFieldEquation . 16 26.3.5 Stellar Models and Their Properties . ..... 18 26.3.6 EmbeddingDiagrams. 19 26.4 Gravitational Implosion of a Star to Form a Black Hole . .......... 22 26.4.1 The Implosion Analyzed in Schwarzschild Coordinates ........ 22 26.4.2 Tidal Forces at the Gravitational Radius . ...... 24 26.4.3 Stellar Implosion in Eddington-Finklestein Coordinates ........ 25 26.4.4 Tidal Forces at r =0 — The Central Singularity . 29 26.4.5 Schwarzschild Black Hole . .. 30 26.5 Spinning Black Holes: The Kerr Spacetime . ....... 35 26.5.1 The Kerr Metric for a Spinning Black Hole . .... 35 26.5.2 DraggingofInertialFrames . .. 36 26.5.3 The Light-Cone Structure, and the Horizon . ..... 37 26.5.4 Evolution of Black Holes — Rotational Energy and Its Extraction . 39 26.6 T2 TheMany-FingeredNatureofTime. 45 0 Chapter 26 Relativistic Stars and Black Holes Version 1326.1.K.pdf, 30 January 2014 Box 26.1 Reader’s Guide This chapter relies significantly on • – Chapter 2 on special relativity.