PHY483F/1483F Relativity Theory I (2020-21) Department of Physics University of Toronto
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2008. Pruning Some Branches from 'Branching Spacetimes'
CHAPTER 10 Pruning Some Branches from “Branching Spacetimes” John Earman* Abstract Discussions of branching time and branching spacetime have become com- mon in the philosophical literature. If properly understood, these concep- tions can be harmless. But they are sometimes used in the service of debat- able and even downright pernicious doctrines. The purpose of this chapter is to identify the pernicious branching and prune it back. 1. INTRODUCTION Talk of “branching time” and “branching spacetime” is wide spread in the philo- sophical literature. Such expressions, if properly understood, can be innocuous. But they are sometimes used in the service of debatable and even downright per- nicious doctrines. The purpose of this paper is to identify the pernicious branching and prune it back. Section 2 distinguishes three types of spacetime branching: individual branch- ing, ensemble branching, and Belnap branching. Individual branching, as the name indicates, involves a branching structure in individual spacetime models. It is argued that such branching is neither necessary nor sufficient for indeterminism, which is explicated in terms of the branching in the ensemble of spacetime mod- els satisfying the laws of physics. Belnap branching refers to the sort of branching used by the Belnap school of branching spacetimes. An attempt is made to sit- uate this sort of branching with respect to ensemble branching and individual branching. Section 3 is a sustained critique of various ways of trying to imple- ment individual branching for relativistic spacetimes. Conclusions are given in Section 4. * Department of History and Philosophy of Science, University of Pittsburgh, Pittsburgh, USA The Ontology of Spacetime II © Elsevier BV ISSN 1871-1774, DOI: 10.1016/S1871-1774(08)00010-7 All rights reserved 187 188 Pruning Some Branches from “Branching Spacetimes” 2. -
Gender and the Quest in British Science Fiction Television CRITICAL EXPLORATIONS in SCIENCE FICTION and FANTASY (A Series Edited by Donald E
Gender and the Quest in British Science Fiction Television CRITICAL EXPLORATIONS IN SCIENCE FICTION AND FANTASY (a series edited by Donald E. Palumbo and C.W. Sullivan III) 1 Worlds Apart? Dualism and Transgression in Contemporary Female Dystopias (Dunja M. Mohr, 2005) 2 Tolkien and Shakespeare: Essays on Shared Themes and Language (ed. Janet Brennan Croft, 2007) 3 Culture, Identities and Technology in the Star Wars Films: Essays on the Two Trilogies (ed. Carl Silvio, Tony M. Vinci, 2007) 4 The Influence of Star Trek on Television, Film and Culture (ed. Lincoln Geraghty, 2008) 5 Hugo Gernsback and the Century of Science Fiction (Gary Westfahl, 2007) 6 One Earth, One People: The Mythopoeic Fantasy Series of Ursula K. Le Guin, Lloyd Alexander, Madeleine L’Engle and Orson Scott Card (Marek Oziewicz, 2008) 7 The Evolution of Tolkien’s Mythology: A Study of the History of Middle-earth (Elizabeth A. Whittingham, 2008) 8 H. Beam Piper: A Biography (John F. Carr, 2008) 9 Dreams and Nightmares: Science and Technology in Myth and Fiction (Mordecai Roshwald, 2008) 10 Lilith in a New Light: Essays on the George MacDonald Fantasy Novel (ed. Lucas H. Harriman, 2008) 11 Feminist Narrative and the Supernatural: The Function of Fantastic Devices in Seven Recent Novels (Katherine J. Weese, 2008) 12 The Science of Fiction and the Fiction of Science: Collected Essays on SF Storytelling and the Gnostic Imagination (Frank McConnell, ed. Gary Westfahl, 2009) 13 Kim Stanley Robinson Maps the Unimaginable: Critical Essays (ed. William J. Burling, 2009) 14 The Inter-Galactic Playground: A Critical Study of Children’s and Teens’ Science Fiction (Farah Mendlesohn, 2009) 15 Science Fiction from Québec: A Postcolonial Study (Amy J. -
Local Flatness and Geodesic Deviation of Causal Geodesics
UTM 724, July 2008 Local flatness and geodesic deviation of causal geodesics. Valter Moretti1,2, Roberto Di Criscienzo3, 1 Dipartimento di Matematica, Universit`adi Trento and Istituto Nazionale di Fisica Nucleare – Gruppo Collegato di Trento, via Sommarive 14 I-38050 Povo (TN), Italy. 2 Istituto Nazionale di Alta Matematica “F.Severi”– GNFM 3 Department of Physics, University of Toronto, 60 St. George Street, Toronto, ON, M5S 1A7, Canada. E-mail: [email protected], [email protected] Abstract. We analyze the interplay of local flatness and geodesic deviation measured for causal geodesics starting from the remark that, form a physical viewpoint, the geodesic deviation can be measured for causal geodesic, observing the motion of (infinitesimal) falling bodies, but it can hardly be evaluated on spacelike geodesics. We establish that a generic spacetime is (locally) flat if and only if there is no geodesic deviation for timelike geodesics or, equivalently, there is no geodesic deviation for null geodesics. 1 Introduction The presence of tidal forces, i.e. geodesic deviation for causal geodesics, can be adopted to give a notion of gravitation valid in the general relativistic context, as the geodesic deviation is not affected by the equivalence principle and thus it cannot be canceled out by an appropriate choice of the reference frame. By direct inspection (see [MTW03]), one sees that the absence of geodesic deviation referred to all type of geodesics is equivalent the fact that the Riemann tensor vanishes everywhere in a spacetime (M, g). The latter fact, in turn, is equivalent to the locally flatness of the spacetime, i.e. -
“Geodesic Principle” in General Relativity∗
A Remark About the “Geodesic Principle” in General Relativity∗ Version 3.0 David B. Malament Department of Logic and Philosophy of Science 3151 Social Science Plaza University of California, Irvine Irvine, CA 92697-5100 [email protected] 1 Introduction General relativity incorporates a number of basic principles that correlate space- time structure with physical objects and processes. Among them is the Geodesic Principle: Free massive point particles traverse timelike geodesics. One can think of it as a relativistic version of Newton’s first law of motion. It is often claimed that the geodesic principle can be recovered as a theorem in general relativity. Indeed, it is claimed that it is a consequence of Einstein’s ∗I am grateful to Robert Geroch for giving me the basic idea for the counterexample (proposition 3.2) that is the principal point of interest in this note. Thanks also to Harvey Brown, Erik Curiel, John Earman, David Garfinkle, John Manchak, Wayne Myrvold, John Norton, and Jim Weatherall for comments on an earlier draft. 1 ab equation (or of the conservation principle ∇aT = 0 that is, itself, a conse- quence of that equation). These claims are certainly correct, but it may be worth drawing attention to one small qualification. Though the geodesic prin- ciple can be recovered as theorem in general relativity, it is not a consequence of Einstein’s equation (or the conservation principle) alone. Other assumptions are needed to drive the theorems in question. One needs to put more in if one is to get the geodesic principle out. My goal in this short note is to make this claim precise (i.e., that other assumptions are needed). -
Geodesic Spheres in Grassmann Manifolds
GEODESIC SPHERES IN GRASSMANN MANIFOLDS BY JOSEPH A. WOLF 1. Introduction Let G,(F) denote the Grassmann manifold consisting of all n-dimensional subspaces of a left /c-dimensional hermitian vectorspce F, where F is the real number field, the complex number field, or the algebra of real quater- nions. We view Cn, (1') tS t Riemnnian symmetric space in the usual way, and study the connected totally geodesic submanifolds B in which any two distinct elements have zero intersection as subspaces of F*. Our main result (Theorem 4 in 8) states that the submanifold B is a compact Riemannian symmetric spce of rank one, and gives the conditions under which it is a sphere. The rest of the paper is devoted to the classification (up to a global isometry of G,(F)) of those submanifolds B which ure isometric to spheres (Theorem 8 in 13). If B is not a sphere, then it is a real, complex, or quater- nionic projective space, or the Cyley projective plane; these submanifolds will be studied in a later paper [11]. The key to this study is the observation thut ny two elements of B, viewed as subspaces of F, are at a constant angle (isoclinic in the sense of Y.-C. Wong [12]). Chapter I is concerned with sets of pairwise isoclinic n-dimen- sional subspces of F, and we are able to extend Wong's structure theorem for such sets [12, Theorem 3.2, p. 25] to the complex numbers nd the qua- ternions, giving a unified and basis-free treatment (Theorem 1 in 4). -
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 . -
3 Spacetime 4 Unitarity Patent Application Publication Mar
US 2012.0075682A1 (19) United States (12) Patent Application Publication (10) Pub. No.: US 2012/0075682 A1 Amoros0 (43) Pub. Date: Mar. 29, 2012 (54) SPACETIME ENERGY RESONATOR: A Publication Classification TRANSISTOR OF COMPLEX DRAC (51) Int. Cl. POLARIZED VACUUM TOPOLOGY GO3H 5/00 (2006.01) B82Y IO/OO (2011.01) (76) Inventor: Richard Louis Amoroso, Oakland, (52) U.S. Cl. ............................................. 359/1977/933 CA (US) (57) ABSTRACT Method and apparatus is described for a general purpose (21) Appl. No.: 12/928,592 transistor of the higher dimensional (HD) spacetime back cloth consistent with symmetry parameters of a new cosmo logical paradigm with a unique M-Theoretic background (22) Filed: Dec. 15, 2010 making correspondence to a complex scale-invariant covari ant Dirac polarized aether where energy pathways follow Related U.S. Application Data spacetime geodesics; and Switching is achieved by manipu lating resonant modes of a Calabi-Yau mirror symmetry hier (60) Provisional application No. 61/284,384, filed on Dec. archy inherent in continuous-State brane topology of the 17, 2009, provisional application No. 61/284,896, structural-phenomenology of least cosmological units tiling filed on Dec. 28, 2009, provisional application No. the raster of spacetime as it emerges from the infinite potential 61/336,522, filed on Jan. 22, 2010. of the unified field. CONCEPTUALIZED NOETIC INTERFEROMETRY Sagnac effect quadrupole modulated RF pulse R2 1 electrons 2 nucleons 3 spacetime 4 unitarity Patent Application Publication Mar. 29, 2012 Sheet 1 of 17 US 2012/0075682 A1 Ring Laser Array Spacetime(S-T)Vacuum Symmetry Hierarchy FIGURE 1 Patent Application Publication Mar. -
General Relativity Fall 2019 Lecture 13: Geodesic Deviation; Einstein field Equations
General Relativity Fall 2019 Lecture 13: Geodesic deviation; Einstein field equations Yacine Ali-Ha¨ımoud October 11th, 2019 GEODESIC DEVIATION The principle of equivalence states that one cannot distinguish a uniform gravitational field from being in an accelerated frame. However, tidal fields, i.e. gradients of gravitational fields, are indeed measurable. Here we will show that the Riemann tensor encodes tidal fields. Consider a fiducial free-falling observer, thus moving along a geodesic G. We set up Fermi normal coordinates in µ the vicinity of this geodesic, i.e. coordinates in which gµν = ηµν jG and ΓνσjG = 0. Events along the geodesic have coordinates (x0; xi) = (t; 0), where we denote by t the proper time of the fiducial observer. Now consider another free-falling observer, close enough from the fiducial observer that we can describe its position with the Fermi normal coordinates. We denote by τ the proper time of that second observer. In the Fermi normal coordinates, the spatial components of the geodesic equation for the second observer can be written as d2xi d dxi d2xi dxi d2t dxi dxµ dxν = (dt/dτ)−1 (dt/dτ)−1 = (dt/dτ)−2 − (dt/dτ)−3 = − Γi − Γ0 : (1) dt2 dτ dτ dτ 2 dτ dτ 2 µν µν dt dt dt The Christoffel symbols have to be evaluated along the geodesic of the second observer. If the second observer is close µ µ λ λ µ enough to the fiducial geodesic, we may Taylor-expand Γνσ around G, where they vanish: Γνσ(x ) ≈ x @λΓνσjG + 2 µ 0 µ O(x ). -
Gravitational Waves and Binary Black Holes
Ondes Gravitationnelles, S´eminairePoincar´eXXII (2016) 1 { 51 S´eminairePoincar´e Gravitational Waves and Binary Black Holes Thibault Damour Institut des Hautes Etudes Scientifiques 35 route de Chartres 91440 Bures sur Yvette, France Abstract. The theoretical aspects of the gravitational motion and radiation of binary black hole systems are reviewed. Several of these theoretical aspects (high-order post-Newtonian equations of motion, high-order post-Newtonian gravitational-wave emission formulas, Effective-One-Body formalism, Numerical-Relativity simulations) have played a significant role in allowing one to compute the 250 000 gravitational-wave templates that were used for search- ing and analyzing the first gravitational-wave events from coalescing binary black holes recently reported by the LIGO-Virgo collaboration. 1 Introduction On February 11, 2016 the LIGO-Virgo collaboration announced [1] the quasi- simultaneous observation by the two LIGO interferometers, on September 14, 2015, of the first Gravitational Wave (GW) event, called GW150914. To set the stage, we show in Figure 1 the raw interferometric data of the event GW150914, transcribed in terms of their equivalent dimensionless GW strain amplitude hobs(t) (Hanford raw data on the left, and Livingston raw data on the right). Figure 1: LIGO raw data for GW150914; taken from the talk of Eric Chassande-Mottin (member of the LIGO-Virgo collaboration) given at the April 5, 2016 public conference on \Gravitational Waves and Coalescing Black Holes" (Acad´emiedes Sciences, Paris, France). The important point conveyed by these plots is that the observed signal hobs(t) (which contains both the noise and the putative real GW signal) is randomly fluc- tuating by ±5 × 10−19 over time scales of ∼ 0:1 sec, i.e. -
The Emergence of Gravitational Wave Science: 100 Years of Development of Mathematical Theory, Detectors, Numerical Algorithms, and Data Analysis Tools
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 53, Number 4, October 2016, Pages 513–554 http://dx.doi.org/10.1090/bull/1544 Article electronically published on August 2, 2016 THE EMERGENCE OF GRAVITATIONAL WAVE SCIENCE: 100 YEARS OF DEVELOPMENT OF MATHEMATICAL THEORY, DETECTORS, NUMERICAL ALGORITHMS, AND DATA ANALYSIS TOOLS MICHAEL HOLST, OLIVIER SARBACH, MANUEL TIGLIO, AND MICHELE VALLISNERI In memory of Sergio Dain Abstract. On September 14, 2015, the newly upgraded Laser Interferometer Gravitational-wave Observatory (LIGO) recorded a loud gravitational-wave (GW) signal, emitted a billion light-years away by a coalescing binary of two stellar-mass black holes. The detection was announced in February 2016, in time for the hundredth anniversary of Einstein’s prediction of GWs within the theory of general relativity (GR). The signal represents the first direct detec- tion of GWs, the first observation of a black-hole binary, and the first test of GR in its strong-field, high-velocity, nonlinear regime. In the remainder of its first observing run, LIGO observed two more signals from black-hole bina- ries, one moderately loud, another at the boundary of statistical significance. The detections mark the end of a decades-long quest and the beginning of GW astronomy: finally, we are able to probe the unseen, electromagnetically dark Universe by listening to it. In this article, we present a short historical overview of GW science: this young discipline combines GR, arguably the crowning achievement of classical physics, with record-setting, ultra-low-noise laser interferometry, and with some of the most powerful developments in the theory of differential geometry, partial differential equations, high-performance computation, numerical analysis, signal processing, statistical inference, and data science. -
+14 Days of Tv Listings Free
CINEMA VOD SPORTS TECH + 14 DAYS OF TV LISTINGS 1 JUNE 2015 ISSUE 2 TVGUIDE.CO.UK TVDAILY.COM Jurassic World Orange is the New Black Formula 1 Addictive Apps FREE 1 JUNE 2015 Issue 2 Contents TVGUIDE.CO.UK TVDAILY.COM EDITOR’S LETTER 4 Latest TV News 17 Food We are living in a The biggest news from the world of television. Your television dinners sorted with revolutionary age for inspiration from our favourite dramas. television. Not only is the way we watch television being challenged by the emergence of video on 18 Travel demand, but what we watch on television is Journey to the dizzying desert of Dorne or becoming increasingly take a trip to see the stunning setting of diverse and, thankfully, starting to catch up with Downton Abbey. real world demographics. With Orange Is The New Black back for another run on Netflix this month, we 19 Fashion decided to celebrate the 6 Top 100 WTF Steal some shadespiration from the arduous journey it’s taken to get to where we are in coolest sunglass-wearing dudes on TV. 2015 (p14). We still have a Moments (Part 2) long way to go, but we’re The final countdown of the most unbelievable getting there. Sports Susan Brett, Editor scenes ever to grace the small screen, 20 including the electrifying number one. All you need to know about the upcoming TVGuide.co.uk Formula 1 and MotoGP races. 104-08 Oxford Street, London, W1D 1LP [email protected] 8 Cinema CONTENT 22 Addictive Apps Editor: Susan Brett Everything you need to know about what’s Deputy Editor: Ally Russell A handy guide to all the best apps for Artistic Director: Francisco on at the Box Office right now.