Scalar Fields in Numerical General Relativity: Inhomogeneous Inflation and Asymmetric Bubble Collapse 3+1D Code Development and Applications
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Numerical Relativity for Vacuum Binary Black Hole Luisa T
Numerical Relativity for Vacuum Binary Black Hole Luisa T. Buchman UW Bothell SXS collaboration (Caltech) Max Planck Institute for Gravitational Physics Albert Einstein Institute GWA NW @ LIGO Hanford Observatory June 25, 2019 Outline • What is numerical relativity? • What is its role in the detection and interpretation of gravitational waves? What is numerical relativity for binary black holes? • 3 stages for binary black hole coalescence: • inspiral • merger • ringdown • Inspiral waveform: Post-Newtonian approximations • Ringdown waveform: perturbation theory • Merger of 2 black holes: • extremely energetic, nonlinear, dynamical and violent • the strongest GW signal • warpage of spacetime • strong gravity regime The Einstein equations: • Gμν = 8πTμν • encodes all of gravity • 10 equations which would take up ~100 pages if no abbreviations or simplifications used (and if written in terms of the spacetime metric alone) • pencil and paper solutions possible only with spherical (Schwarzschild) or axisymmetric (Kerr) symmetries. • Vacuum: G = 0 μν (empty space with no matter) Numerical Relativity is: • Directly solving the full dynamical Einstein field equations using high-performance computing. • A very difficult problem: • the first attempts at numerical simulations of binary black holes was in the 1960s (Hahn and Lindquist) and mid-1970s (Smarr and others). • the full 3D problem remained unsolved until 2005 (Frans Pretorius, followed quickly by 2 other groups- Campanelli et al., Baker et al.). Solving Einstein’s Equations on a Computer • -
Modified Julian Date Timing Residual
NEWSLETTER February 2015 Issue no. 10 0.003 0.002 0.001 0.000 Timing residual [s] 0.001 − 0.002 − 45000 45500 46000 46500 47000 Modified Julian Date The timing residual (difference between the measured times of arrival of pulses and the timing model) for the crab pulsar, collected using data from the Crab ephermis. Figure courtesy G. Ashton See http://gp.iop.org for more details Gravitational Physics Group February 2015 Table of Contents Welcome from the Chair .................................................... 3 Events ................................................................................ 5 Young Theorists’ Forum 2013 ......................................................................... 5 New Frontiers in Dynamical Gravity ............................................................... 5 BritGrav 2014 .................................................................................................... 6 Prizes ................................................................................. 8 2014 GPG Thesis Prize .................................................................................... 8 Contributed Articles ........................................................... 9 The effect of timing noise on continuous gravitational wave searches ..... 9 Black holes and scalar hair ........................................................................... 17 Untangling precession: Modelling the gravitational wave signal from precessing black hole binaries .................................................................... -
An Introduction to Quantum Field Theory
AN INTRODUCTION TO QUANTUM FIELD THEORY By Dr M Dasgupta University of Manchester Lecture presented at the School for Experimental High Energy Physics Students Somerville College, Oxford, September 2009 - 1 - - 2 - Contents 0 Prologue....................................................................................................... 5 1 Introduction ................................................................................................ 6 1.1 Lagrangian formalism in classical mechanics......................................... 6 1.2 Quantum mechanics................................................................................... 8 1.3 The Schrödinger picture........................................................................... 10 1.4 The Heisenberg picture............................................................................ 11 1.5 The quantum mechanical harmonic oscillator ..................................... 12 Problems .............................................................................................................. 13 2 Classical Field Theory............................................................................. 14 2.1 From N-point mechanics to field theory ............................................... 14 2.2 Relativistic field theory ............................................................................ 15 2.3 Action for a scalar field ............................................................................ 15 2.4 Plane wave solution to the Klein-Gordon equation ........................... -
Towards a Gauge Polyvalent Numerical Relativity Code: Numerical Methods, Boundary Conditions and Different Formulations
UNIVERSITAT DE LES ILLES BALEARS Towards a gauge polyvalent numerical relativity code: numerical methods, boundary conditions and different formulations per Carles Bona-Casas Tesi presentada per a l'obtenci´o del t´ıtolde doctor a la Facultat de Ci`encies Departament de F´ısica Dirigida per: Prof. Carles Bona Garcia i Dr. Joan Mass´oBenn`assar "The fact that we live at the bottom of a deep gravity well, on the surface of a gas covered planet going around a nuclear fireball 90 million miles away and think this to be normal is obviously some indication of how skewed our perspective tends to be." Douglas Adams. Acknowledgements I would like to acknowledge everyone who ever taught me something. Specially my supervisors who, at least in the beginning, had to suffer my eyes, puzzling at their faces, saying that I had the impression that what they were explaining to me was some unreachable knowledge. It turns out that there is not such a thing and they have finally managed to make me gain some insight in this world of relativity and computing. They have also infected me the disease of worrying about calculations and stuff that most people wouldn't care about and my hair doesn't seem very happy with it, but I still love them for that. Many thanks to everyone in the UIB relativity group and to all the PhD. students who have shared some time with me. Work is less hard in their company. Special thanks to Carlos, Denis, Sasha and Dana for all their very useful comments and for letting me play with their work and codes. -
Exact Solutions to the Interacting Spinor and Scalar Field Equations in the Godel Universe
XJ9700082 E2-96-367 A.Herrera 1, G.N.Shikin2 EXACT SOLUTIONS TO fHE INTERACTING SPINOR AND SCALAR FIELD EQUATIONS IN THE GODEL UNIVERSE 1 E-mail: [email protected] ^Department of Theoretical Physics, Russian Peoples ’ Friendship University, 117198, 6 Mikluho-Maklaya str., Moscow, Russia ^8 as ^; 1996 © (XrbCAHHeHHuft HHCTtrryr McpHMX HCCJicAOB&Htift, fly 6na, 1996 1. INTRODUCTION Recently an increasing interest was expressed to the search of soliton-like solu tions because of the necessity to describe the elementary particles as extended objects [1]. In this work, the interacting spinor and scalar field system is considered in the external gravitational field of the Godel universe in order to study the influence of the global properties of space-time on the interaction of one dimensional fields, in other words, to observe what is the role of gravitation in the interaction of elementary particles. The Godel universe exhibits a number of unusual properties associated with the rotation of the universe [2]. It is ho mogeneous in space and time and is filled with a perfect fluid. The main role of rotation in this universe consists in the avoidance of the cosmological singu larity in the early universe, when the centrifugate forces of rotation dominate over gravitation and the collapse does not occur [3]. The paper is organized as follows: in Sec. 2 the interacting spinor and scalar field system with £jnt = | <ptp<p'PF(Is) in the Godel universe is considered and exact solutions to the corresponding field equations are obtained. In Sec. 3 the properties of the energy density are investigated. -
Numerical Relativity
Paper presented at the 13th Int. Conf on General Relativity and Gravitation 373 Cordoba, Argentina, 1992: Part 2, Workshop Summaries Numerical relativity Takashi Nakamura Yulcawa Institute for Theoretical Physics, Kyoto University, Kyoto 606, JAPAN In GR13 we heard many reports on recent. progress as well as future plans of detection of gravitational waves. According to these reports (see the report of the workshop on the detection of gravitational waves by Paik in this volume), it is highly probable that the sensitivity of detectors such as laser interferometers and ultra low temperature resonant bars will reach the level of h ~ 10—21 by 1998. in this level we may expect the detection of the gravitational waves from astrophysical sources such as coalescing binary neutron stars once a year or so. Therefore the progress in numerical relativity is urgently required to predict the wave pattern and amplitude of the gravitational waves from realistic astrophysical sources. The time left for numerical relativists is only six years or so although there are so many difficulties in principle as well as in practice. Apart from detection of gravitational waves, numerical relativity itself has a final goal: Solve the Einstein equations numerically for (my initial data as accurately as possible and clarify physics in strong gravity. in GRIIS there were six oral presentations and ll poster papers on recent progress in numerical relativity. i will make a brief review of six oral presenta— tions. The Regge calculus is one of methods to investigate spacetimes numerically. Brewin from Monash University Australia presented a paper Particle Paths in a Schwarzshild Spacetime via. -
An Introduction to Supersymmetry
An Introduction to Supersymmetry Ulrich Theis Institute for Theoretical Physics, Friedrich-Schiller-University Jena, Max-Wien-Platz 1, D–07743 Jena, Germany [email protected] This is a write-up of a series of five introductory lectures on global supersymmetry in four dimensions given at the 13th “Saalburg” Summer School 2007 in Wolfersdorf, Germany. Contents 1 Why supersymmetry? 1 2 Weyl spinors in D=4 4 3 The supersymmetry algebra 6 4 Supersymmetry multiplets 6 5 Superspace and superfields 9 6 Superspace integration 11 7 Chiral superfields 13 8 Supersymmetric gauge theories 17 9 Supersymmetry breaking 22 10 Perturbative non-renormalization theorems 26 A Sigma matrices 29 1 Why supersymmetry? When the Large Hadron Collider at CERN takes up operations soon, its main objective, besides confirming the existence of the Higgs boson, will be to discover new physics beyond the standard model of the strong and electroweak interactions. It is widely believed that what will be found is a (at energies accessible to the LHC softly broken) supersymmetric extension of the standard model. What makes supersymmetry such an attractive feature that the majority of the theoretical physics community is convinced of its existence? 1 First of all, under plausible assumptions on the properties of relativistic quantum field theories, supersymmetry is the unique extension of the algebra of Poincar´eand internal symmtries of the S-matrix. If new physics is based on such an extension, it must be supersymmetric. Furthermore, the quantum properties of supersymmetric theories are much better under control than in non-supersymmetric ones, thanks to powerful non- renormalization theorems. -
Curriculum Vitae
Christopher Berry Personal Department Address Email Telephone Information School of Physics & Astronomy [email protected] +44 (0) 1214 146541 University of Birmingham Edgbaston Website Twitter Birmingham cplberry.com @cplberry B15 2TT Education University of Birmingham September 2014 { April 2015 PGCert (Associate Module) Foundation of Learning & Teaching in Higher Education Institute of Astronomy, University of Cambridge October 2009 { August 2013 PhD in Astronomy Supervisor: Jonathan Gair Exploring gravity with strong-field tests and gravitational waves. Theoretical study of what can be learned about astrophysical systems and the nature of gravity from gravitational probes, in particular gravitational waves. Funded by STFC and the Cambridge Philosophical Society. Churchill College, University of Cambridge October 2005 { July 2009 BA (Hons), MSci Natural Sciences Part III Experimental & Theoretical Physics 1st Part II Experimental & Theoretical Physics 1st Part IB Physics, Advanced Physics, Mathematics 1st Part IA Physics, Materials & Mineral Science, Geology, Mathematics 1st Worcester College of Technology September 2004 { June 2005 Certificate in Management (Level 3) Distinction Introductory Certificate in Management (Level 3) Distinction Droitwich Spa High School & Sixth Form Centre September 1998 { June 2004 STEP Mathematics II, Mathematics III 1 A-level Physics, Maths, Further Maths, General Studies A AS-level Geography A GCSE 10 (including Maths, English and French) 9 A*s, 1 A Honours, Awards 2018 IOP Astroparticle Physics Early -
Vector Fields
Vector Calculus Independent Study Unit 5: Vector Fields A vector field is a function which associates a vector to every point in space. Vector fields are everywhere in nature, from the wind (which has a velocity vector at every point) to gravity (which, in the simplest interpretation, would exert a vector force at on a mass at every point) to the gradient of any scalar field (for example, the gradient of the temperature field assigns to each point a vector which says which direction to travel if you want to get hotter fastest). In this section, you will learn the following techniques and topics: • How to graph a vector field by picking lots of points, evaluating the field at those points, and then drawing the resulting vector with its tail at the point. • A flow line for a velocity vector field is a path ~σ(t) that satisfies ~σ0(t)=F~(~σ(t)) For example, a tiny speck of dust in the wind follows a flow line. If you have an acceleration vector field, a flow line path satisfies ~σ00(t)=F~(~σ(t)) [For example, a tiny comet being acted on by gravity.] • Any vector field F~ which is equal to ∇f for some f is called a con- servative vector field, and f its potential. The terminology comes from physics; by the fundamental theorem of calculus for work in- tegrals, the work done by moving from one point to another in a conservative vector field doesn’t depend on the path and is simply the difference in potential at the two points. -
The Initial Data Problem for 3+1 Numerical Relativity Part 2
The initial data problem for 3+1 numerical relativity Part 2 Eric Gourgoulhon Laboratoire Univers et Th´eories (LUTH) CNRS / Observatoire de Paris / Universit´eParis Diderot F-92190 Meudon, France [email protected] http://www.luth.obspm.fr/∼luthier/gourgoulhon/ 2008 International Summer School on Computational Methods in Gravitation and Astrophysics Asia Pacific Center for Theoretical Physics, Pohang, Korea 28 July - 1 August 2008 Eric Gourgoulhon (LUTH) Initial data problem 2 / 2 APCTP School, 31 July 2008 1 / 41 Plan 1 Helical symmetry for binary systems 2 Initial data for orbiting binary black holes 3 Initial data for orbiting binary neutron stars 4 Initial data for orbiting black hole - neutron star systems 5 References for lectures 1-3 Eric Gourgoulhon (LUTH) Initial data problem 2 / 2 APCTP School, 31 July 2008 2 / 41 Helical symmetry for binary systems Outline 1 Helical symmetry for binary systems 2 Initial data for orbiting binary black holes 3 Initial data for orbiting binary neutron stars 4 Initial data for orbiting black hole - neutron star systems 5 References for lectures 1-3 Eric Gourgoulhon (LUTH) Initial data problem 2 / 2 APCTP School, 31 July 2008 3 / 41 Helical symmetry for binary systems Helical symmetry for binary systems Physical assumption: when the two objects are sufficiently far apart, the radiation reaction can be neglected ⇒ closed orbits Gravitational radiation reaction circularizes the orbits ⇒ circular orbits Geometrical translation: spacetime possesses some helical symmetry Helical Killing vector ξ: -
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 . -
TASI 2008 Lectures: Introduction to Supersymmetry And
TASI 2008 Lectures: Introduction to Supersymmetry and Supersymmetry Breaking Yuri Shirman Department of Physics and Astronomy University of California, Irvine, CA 92697. [email protected] Abstract These lectures, presented at TASI 08 school, provide an introduction to supersymmetry and supersymmetry breaking. We present basic formalism of supersymmetry, super- symmetric non-renormalization theorems, and summarize non-perturbative dynamics of supersymmetric QCD. We then turn to discussion of tree level, non-perturbative, and metastable supersymmetry breaking. We introduce Minimal Supersymmetric Standard Model and discuss soft parameters in the Lagrangian. Finally we discuss several mech- anisms for communicating the supersymmetry breaking between the hidden and visible sectors. arXiv:0907.0039v1 [hep-ph] 1 Jul 2009 Contents 1 Introduction 2 1.1 Motivation..................................... 2 1.2 Weylfermions................................... 4 1.3 Afirstlookatsupersymmetry . .. 5 2 Constructing supersymmetric Lagrangians 6 2.1 Wess-ZuminoModel ............................... 6 2.2 Superfieldformalism .............................. 8 2.3 VectorSuperfield ................................. 12 2.4 Supersymmetric U(1)gaugetheory ....................... 13 2.5 Non-abeliangaugetheory . .. 15 3 Non-renormalization theorems 16 3.1 R-symmetry.................................... 17 3.2 Superpotentialterms . .. .. .. 17 3.3 Gaugecouplingrenormalization . ..... 19 3.4 D-termrenormalization. ... 20 4 Non-perturbative dynamics in SUSY QCD 20 4.1 Affleck-Dine-Seiberg