General Relativistic Collapse of Rotating Stellar Cores in Axisymmetry
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Covariant Hamiltonian Formalism for Field Theory: Hamilton-Jacobi
Covariant hamiltonian formalism for field theory: Hamilton-Jacobi equation on the space G Carlo Rovelli Centre de Physique Th´eorique de Luminy, CNRS, Case 907, F-13288 Marseille, EU February 7, 2008 Abstract Hamiltonian mechanics of field theory can be formulated in a generally covariant and background independent manner over a finite dimensional extended configuration space. The physical symplectic structure of the theory can then be defined over a space G of three-dimensional surfaces without boundary, in the extended configuration space. These surfaces provide a preferred over-coordinatization of phase space. I consider the covariant form of the Hamilton-Jacobi equation on G, and a canonical function S on G which is a preferred solution of the Hamilton-Jacobi equation. The application of this formalism to general relativity is equiv- alent to the ADM formalism, but fully covariant. In the quantum domain, it yields directly the Ashtekar-Wheeler-DeWitt equation. Finally, I apply this formalism to discuss the partial observables of a covariant field theory and the role of the spin networks –basic objects in quantum gravity– in the classical theory. arXiv:gr-qc/0207043v2 26 Jul 2002 1 Introduction Hamiltonian mechanics is a clean and general formalism for describing a physi- cal system, its states and its observables, and provides a road towards quantum theory. In its traditional formulation, however, the hamiltonian formalism is badly non covariant. This is a source of problems already for finite dimensional systems. For instance, the notions of state and observable are not very clean in the hamiltonian mechanics of the systems where evolution is given in para- metric form, especially if the evolution cannot be deparametrized (as in certain cosmological models). -
Linearization Instability in Gravity Theories1
Linearization Instability in Gravity Theories1 Emel Altasa;2 a Department of Physics, Middle East Technical University, 06800, Ankara, Turkey. Abstract In a nonlinear theory, such as gravity, physically relevant solutions are usually hard to find. Therefore, starting from a background exact solution with symmetries, one uses the perturbation theory, which albeit approximately, provides a lot of information regarding a physical solution. But even this approximate information comes with a price: the basic premise of a perturbative solution is that it should be improvable. Namely, by going to higher order perturbation theory, one should be able to improve and better approximate the physical problem or the solution. While this is often the case in many theories and many background solutions, there are important cases where the linear perturbation theory simply fails for various reasons. This issue is well known in the context of general relativity through the works that started in the early 1970s, but it has only been recently studied in modified gravity theories. This thesis is devoted to the study of linearization instability in generic gravity theories where there are spurious solutions to the linearized equations which do not come from the linearization of possible exact solutions. For this purpose we discuss the Taub charges, arXiv:1808.04722v2 [hep-th] 2 Sep 2018 the ADT charges and the quadratic constraints on the linearized solutions. We give the three dimensional chiral gravity and the D dimensional critical gravity as explicit examples and give a detailed ADM analysis of the topologically massive gravity with a cosmological constant. 1This is a Ph.D. -
Wave Extraction in Numerical Relativity
Doctoral Dissertation Wave Extraction in Numerical Relativity Dissertation zur Erlangung des naturwissenschaftlichen Doktorgrades der Bayrischen Julius-Maximilians-Universitat¨ Wurzburg¨ vorgelegt von Oliver Elbracht aus Warendorf Institut fur¨ Theoretische Physik und Astrophysik Fakultat¨ fur¨ Physik und Astronomie Julius-Maximilians-Universitat¨ Wurzburg¨ Wurzburg,¨ August 2009 Eingereicht am: 27. August 2009 bei der Fakultat¨ fur¨ Physik und Astronomie 1. Gutachter:Prof.Dr.Karl Mannheim 2. Gutachter:Prof.Dr.Thomas Trefzger 3. Gutachter:- der Dissertation. 1. Prufer¨ :Prof.Dr.Karl Mannheim 2. Prufer¨ :Prof.Dr.Thomas Trefzger 3. Prufer¨ :Prof.Dr.Thorsten Ohl im Promotionskolloquium. Tag des Promotionskolloquiums: 26. November 2009 Doktorurkunde ausgehandigt¨ am: Gewidmet meinen Eltern, Gertrud und Peter, f¨urall ihre Liebe und Unterst¨utzung. To my parents Gertrud and Peter, for all their love, encouragement and support. Wave Extraction in Numerical Relativity Abstract This work focuses on a fundamental problem in modern numerical rela- tivity: Extracting gravitational waves in a coordinate and gauge independent way to nourish a unique and physically meaningful expression. We adopt a new procedure to extract the physically relevant quantities from the numerically evolved space-time. We introduce a general canonical form for the Weyl scalars in terms of fundamental space-time invariants, and demonstrate how this ap- proach supersedes the explicit definition of a particular null tetrad. As a second objective, we further characterize a particular sub-class of tetrads in the Newman-Penrose formalism: the transverse frames. We establish a new connection between the two major frames for wave extraction: namely the Gram-Schmidt frame, and the quasi-Kinnersley frame. Finally, we study how the expressions for the Weyl scalars depend on the tetrad we choose, in a space-time containing distorted black holes. -
Rotating Stars in Relativity
Noname manuscript No. (will be inserted by the editor) Rotating Stars in Relativity Vasileios Paschalidis Nikolaos Stergioulas · Received: date / Accepted: date Abstract Rotating relativistic stars have been studied extensively in recent years, both theoretically and observationally, because of the information they might yield about the equation of state of matter at extremely high densi- ties and because they are considered to be promising sources of gravitational waves. The latest theoretical understanding of rotating stars in relativity is re- viewed in this updated article. The sections on equilibrium properties and on nonaxisymmetric oscillations and instabilities in f-modes and r-modes have been updated. Several new sections have been added on equilibria in modi- fied theories of gravity, approximate universal relationships, the one-arm spiral instability, on analytic solutions for the exterior spacetime, rotating stars in LMXBs, rotating strange stars, and on rotating stars in numerical relativ- ity including both hydrodynamic and magnetohydrodynamic studies of these objects. Keywords Relativistic stars · Rotation · Stability · Oscillations · Magnetic fields · Numerical relativity Vasileios Paschalidis Theoretical Astrophysics Program, Departments of Astronomy and Physics, University of Arizona, Tucson, AZ 85721, USA Department of Physics, Princeton University Princeton, NJ 08544, USA E-mail: [email protected] http://physics.princeton.edu/~vp16/ Nikolaos Stergioulas Department of Physics, Aristotle University of Thessaloniki Thessaloniki, 54124, Greece E-mail: [email protected] http://www.astro.auth.gr/~niksterg arXiv:1612.03050v2 [astro-ph.HE] 30 Nov 2017 2 Vasileios Paschalidis, Nikolaos Stergioulas The article has been substantially revised and updated. New Section 5 and various Subsections (2.3 { 2.5, 2.7.5 { 2.7.7, 2.8, 2.10-2.11,4.5.7) have been added. -
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 . -
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. -
Arxiv:1912.00685V2 [Gr-Qc] 30 Mar 2020
USTC-ICTS-19-29 Relativistic stars in mass-varying massive gravity Xue Sun1 and Shuang-Yong Zhou2 1School of Physical Sciences, University of Science and Technology of China, Hefei, Anhui 230026, China 2Interdisciplinary Center for Theoretical Study, University of Science and Technology of China, Hefei, Anhui 230026, China and Peng Huanwu Center for Fundamental Theory, Hefei, Anhui 230026, China (Dated: March 31, 2020) Mass-varying massive gravity allows the graviton mass to vary according to different environ- ments. We investigate neutron star and white dwarf solutions in this theory and find that the graviton mass can become very large near the compact stars and settle down quickly to small cosmological values away the stars, similar to that of black holes in the theory. It is found that there exists a tower of compact star solutions where the graviton mass decreases radially to zero non-trivially. We compute the massive graviton effects on the mass-radius relations of the compact stars, and also compare the relative strengths between neutron stars and white dwarfs in constraining the parameter space of mass-varying massive gravity. I. INTRODUCTION ton mass near the horizon, there is an extra potential barrier to the left of the photosphere barrier in the mod- ified Regge-Wheeler-Zerilli equation, and this can lead to Recent advances in astrophysics, particularly the ar- gravitational wave echoes [18, 19] in the late time ring- rival of gravitational wave astronomy [1, 2], have pro- down waveform when the black hole is perturbed [16]. vided fresh new opportunities to test gravity in the strong field regime with compact astronomical objects. -
Relativistic Stars with a Linear Equation of State: Analogy with Classical Isothermal Spheres and Black Holes
A&A 483, 673–698 (2008) Astronomy DOI: 10.1051/0004-6361:20078287 & c ESO 2008 Astrophysics Relativistic stars with a linear equation of state: analogy with classical isothermal spheres and black holes P. H. Chavanis Laboratoire de Physique Théorique (UMR 5152 du CNRS), Université Paul Sabatier, 118 route de Narbonne, 31062 Toulouse, France e-mail: [email protected] Received 16 July 2007 / Accepted 10 February 2008 ABSTRACT We complete our previous investigations concerning the structure and the stability of “isothermal” spheres in general relativity. This concerns objects that are described by a linear equation of state, P = q, so that the pressure is proportional to the energy density. In the Newtonian limit q → 0, this returns the classical isothermal equation of state. We specifically consider a self-gravitating radiation (q = 1/3), the core of neutron stars (q = 1/3), and a gas of baryons interacting through a vector meson field (q = 1). Inspired by recent works, we study how the thermodynamical parameters (entropy, temperature, baryon number, mass-energy, etc.) scale with the size of the object and find unusual behaviours due to the non-extensivity of the system. We compare these scaling laws with the area scaling of the black hole entropy. We also determine the domain of validity of these scaling laws by calculating the critical radius (for a given central density) above which relativistic stars described by a linear equation of state become dynamically unstable. For photon stars (self-gravitating radiation), we show that the criteria of dynamical and thermodynamical stability coincide. Considering finite spheres, we find that the mass and entropy present damped oscillations as a function of the central density. -
Extraction of Gravitational Waves in Numerical Relativity
Extraction of Gravitational Waves in Numerical Relativity Nigel T. Bishop Department of Mathematics, Rhodes University, Grahamstown 6140, South Africa email: [email protected] http://www.ru.ac.za/mathematics/people/staff/nigelbishop Luciano Rezzolla Institute for Theoretical Physics, 60438 Frankfurt am Main, Germany Frankfurt Institute for Advanced Studies, 60438 Frankfurt am Main, Germany email: [email protected] http://astro.uni-frankfurt.de/rezzolla July 5, 2016 Abstract A numerical-relativity calculation yields in general a solution of the Einstein equations including also a radiative part, which is in practice computed in a region of finite extent. Since gravitational radiation is properly defined only at null infinity and in an appropriate coordinate system, the accurate estimation of the emitted gravitational waves represents an old and non-trivial problem in numerical relativity. A number of methods have been developed over the years to \extract" the radiative part of the solution from a numerical simulation and these include: quadrupole formulas, gauge-invariant metric perturbations, Weyl scalars, and characteristic extraction. We review and discuss each method, in terms of both its theoretical background as well as its implementation. Finally, we provide a brief comparison of the various methods in terms of their inherent advantages and disadvantages. arXiv:1606.02532v2 [gr-qc] 4 Jul 2016 1 Contents 1 Introduction 4 2 A Quick Review of Gravitational Waves6 2.1 Linearized Einstein equations . .6 2.2 Making sense of the TT gauge . .9 2.3 The quadrupole formula . 12 2.3.1 Extensions of the quadrupole formula . 14 3 Basic Numerical Approaches 17 3.1 The 3+1 decomposition of spacetime . -
ADM Formalism with G and Λ Variable
Outline of the talk l Quantum Gravity and Asymptotic Safety in Q.G. l Brief description of Lorentian Asymptotic Safety l ADM formalism with G and Λ variable. l Cosmologies of the Sub-Planck era l Bouncing and Emergent Universes. l Conclusions. QUANTUM GRAVITY l Einstein General Relativity works quite well for distances l≫lPl (=Planck lenght). l Singularity problem and the quantum mechanical behavour of matter-energy at small distance suggest a quantum mechanical behavour of the gravitational field (Quantum Gravity) at small distances (High Energy). l Many different approaches to Quantum Gravity: String Theory, Loop Quantum Gravity, Non-commutative Geometry, CDT, Asymptotic Safety etc. l General Relativity is considered an effective theory. It is not pertubatively renormalizable (the Newton constant G has a (lenght)-2 dimension) QUANTUM GRAVITY l Fundamental theories (in Quantum Field Theory), in general, are believed to be perturbatively renormalizable. Their infinities can be absorbed by redefining their parameters (m,g,..etc). l Perturbative non-renormalizability: the number of counter terms increase as the loops orders do, then there are infinitely many parameters and no- predictivity of the theory. l There exist fundamental (=infinite cut off limit) theories which are not “perturbatively non renormalizable (along the line of Wilson theory of renormalization). l They are constructed by taking the infinite-cut off limit (continuum limit) at a non-Gaussinan fixed point (u* ≠ 0, pert. Theories have trivial Gaussian point u* = 0). ASYMPTOTIC SAFETY l The “Asymptotic safety” conjecture of Weinberg (1979) suggest to run the coupling constants of the theory, find a non (NGFP)-Gaussian fixed point in this space of parameters, define the Quantum theory at this point. -
A Semiclassical Intrinsic Canonical Approach to Quantum Gravity
Semi-classical Intrinsic Gravity A semiclassical intrinsic canonical approach to quantum gravity J¨urgenRenn∗ and Donald Salisbury+ Austin College, Texas+ Max Planck Institute for the History of Science, Berlin+∗ Reflections on the Quantum Nature of Space and Time Albert Einstein Institute, Golm, Germany, November 28, 2012 Semi-classical Intrinsic Gravity Overview 1 Introduction 2 An historically motivated heuristics 3 The standard approach to semiclassical canonical quantization 4 Limitations of the standard approach to semiclassical canonical quantization 5 History of constrained Hamiltonian dynamics 6 A bridge between spacetime and phase space formulations of general relativity 7 Intrinsic coordinates and a Hamilton-Jacobi approach to semi-classical quantum gravity Semi-classical Intrinsic Gravity Introduction 1. INTRODUCTION Semi-classical Intrinsic Gravity Introduction Introduction The twentieth century founders of quantum mechanics drew on a rich classical mechanical tradition in their effort to incorporate the quantum of action into their deliberations. The phase space formulation of mechanics proved to be the most amenable to adaptation, and in fact the resulting quantum theory proved to not be so distant from the classical theory within the framework of the associated Hamilton-Jacobi theory. Semi-classical Intrinsic Gravity Introduction Introduction We will briefly review these efforts and their relevance to attempts over the past few decades to construct a quantum theory of gravity. We emphasize in our overview the heuristic role of the action, and in referring to observations of several of the historically important players we witness frequent expressions of hope, but also misgivings and even misunderstandings that have arisen in attempts to apply Hamilton-Jacobi techniques in a semi-classical approach to quantum gravity. -
Post-Newtonian Approximations and Applications
Monash University MTH3000 Research Project Coming out of the woodwork: Post-Newtonian approximations and applications Author: Supervisor: Justin Forlano Dr. Todd Oliynyk March 25, 2015 Contents 1 Introduction 2 2 The post-Newtonian Approximation 5 2.1 The Relaxed Einstein Field Equations . 5 2.2 Solution Method . 7 2.3 Zones of Integration . 13 2.4 Multi-pole Expansions . 15 2.5 The first post-Newtonian potentials . 17 2.6 Alternate Integration Methods . 24 3 Equations of Motion and the Precession of Mercury 28 3.1 Deriving equations of motion . 28 3.2 Application to precession of Mercury . 33 4 Gravitational Waves and the Hulse-Taylor Binary 38 4.1 Transverse-traceless potentials and polarisations . 38 4.2 Particular gravitational wave fields . 42 4.3 Effect of gravitational waves on space-time . 46 4.4 Quadrupole formula . 48 4.5 Application to Hulse-Taylor binary . 52 4.6 Beyond the Quadrupole formula . 56 5 Concluding Remarks 58 A Appendix 63 A.1 Solving the Wave Equation . 63 A.2 Angular STF Tensors and Spherical Averages . 64 A.3 Evaluation of a 1PN surface integral . 65 A.4 Details of Quadrupole formula derivation . 66 1 Chapter 1 Introduction Einstein's General theory of relativity [1] was a bold departure from the widely successful Newtonian theory. Unlike the Newtonian theory written in terms of fields, gravitation is a geometric phenomena, with space and time forming a space-time manifold that is deformed by the presence of matter and energy. The deformation of this differentiable manifold is characterised by a symmetric metric, and freely falling (not acted on by exter- nal forces) particles will move along geodesics of this manifold as determined by the metric.