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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). -
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. -
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. -
Laplacians in Geometric Analysis
LAPLACIANS IN GEOMETRIC ANALYSIS Syafiq Johar syafi[email protected] Contents 1 Trace Laplacian 1 1.1 Connections on Vector Bundles . .1 1.2 Local and Explicit Expressions . .2 1.3 Second Covariant Derivative . .3 1.4 Curvatures on Vector Bundles . .4 1.5 Trace Laplacian . .5 2 Harmonic Functions 6 2.1 Gradient and Divergence Operators . .7 2.2 Laplace-Beltrami Operator . .7 2.3 Harmonic Functions . .8 2.4 Harmonic Maps . .8 3 Hodge Laplacian 9 3.1 Exterior Derivatives . .9 3.2 Hodge Duals . 10 3.3 Hodge Laplacian . 12 4 Hodge Decomposition 13 4.1 De Rham Cohomology . 13 4.2 Hodge Decomposition Theorem . 14 5 Weitzenb¨ock and B¨ochner Formulas 15 5.1 Weitzenb¨ock Formula . 15 5.1.1 0-forms . 15 5.1.2 k-forms . 15 5.2 B¨ochner Formula . 17 1 Trace Laplacian In this section, we are going to present a notion of Laplacian that is regularly used in differential geometry, namely the trace Laplacian (also called the rough Laplacian or connection Laplacian). We recall the definition of connection on vector bundles which allows us to take the directional derivative of vector bundles. 1.1 Connections on Vector Bundles Definition 1.1 (Connection). Let M be a differentiable manifold and E a vector bundle over M. A connection or covariant derivative at a point p 2 M is a map D : Γ(E) ! Γ(T ∗M ⊗ E) 1 with the properties for any V; W 2 TpM; σ; τ 2 Γ(E) and f 2 C (M), we have that DV σ 2 Ep with the following properties: 1. -
Symmetries and Pre-Metric Electromagnetism
Symmetries and pre-metric electromagnetism ∗ D.H. Delphenich ∗∗ Physics Department, Bethany College, Lindsborg, KS 67456, USA Received 27 April 2005, revised 14 July 2005, accepted 14 July 2005 by F. W. Hehl Key words Pre-metric electromagnetism, exterior differential systems, symmetries of differential equations, electromagnetic constitutive laws, projective relativity. PACS 02.40.k, 03.50.De, 11.30-j, 11.10-Lm The equations of pre-metric electromagnetism are formulated as an exterior differential system on the bundle of exterior differential 2-forms over the spacetime manifold. The general form for the symmetry equations of the system is computed and then specialized to various possible forms for an electromagnetic constitutive law, namely, uniform linear, non-uniform linear, and uniform nonlinear. It is shown that in the uniform linear case, one has four possible ways of prolonging the symmetry Lie algebra, including prolongation to a Lie algebra of infinitesimal projective transformations of a real four-dimensional projective space. In the most general non-uniform linear case, the effect of non-uniformity on symmetry seems inconclusive in the absence of further specifics, and in the uniform nonlinear case, the overall difference from the uniform linear case amounts to a deformation of the electromagnetic constitutive tensor by the electromagnetic field strengths, which induces a corresponding deformation of the symmetry Lie algebra that was obtained in the linear uniform case. Contents 1 Introduction 2 2 Exterior differential systems 4 2.1 Basic concepts. ………………………………………………………………………….. 4 2.2 Exterior differential systems on Λ2(M). …………………………………………………. 6 2.3 Canonical forms on Λ2(M). ………………………………………………………………. 7 3. Symmetries of exterior differential systems 10 3.1 Basic concepts. -
Selected Papers on Teleparallelism Ii
SELECTED PAPERS ON TELEPARALLELISM Edited and translated by D. H. Delphenich Table of contents Page Introduction ……………………………………………………………………… 1 1. The unification of gravitation and electromagnetism 1 2. The geometry of parallelizable manifold 7 3. The field equations 20 4. The topology of parallelizability 24 5. Teleparallelism and the Dirac equation 28 6. Singular teleparallelism 29 References ……………………………………………………………………….. 33 Translations and time line 1928: A. Einstein, “Riemannian geometry, while maintaining the notion of teleparallelism ,” Sitzber. Preuss. Akad. Wiss. 17 (1928), 217- 221………………………………………………………………………………. 35 (Received on June 7) A. Einstein, “A new possibility for a unified field theory of gravitation and electromagnetism” Sitzber. Preuss. Akad. Wiss. 17 (1928), 224-227………… 42 (Received on June 14) R. Weitzenböck, “Differential invariants in EINSTEIN’s theory of teleparallelism,” Sitzber. Preuss. Akad. Wiss. 17 (1928), 466-474……………… 46 (Received on Oct 18) 1929: E. Bortolotti , “ Stars of congruences and absolute parallelism: Geometric basis for a recent theory of Einstein ,” Rend. Reale Acc. dei Lincei 9 (1929), 530- 538...…………………………………………………………………………….. 56 R. Zaycoff, “On the foundations of a new field theory of A. Einstein,” Zeit. Phys. 53 (1929), 719-728…………………………………………………............ 64 (Received on January 13) Hans Reichenbach, “On the classification of the new Einstein Ansatz on gravitation and electricity,” Zeit. Phys. 53 (1929), 683-689…………………….. 76 (Received on January 22) Selected papers on teleparallelism ii A. Einstein, “On unified field theory,” Sitzber. Preuss. Akad. Wiss. 18 (1929), 2-7……………………………………………………………………………….. 82 (Received on Jan 30) R. Zaycoff, “On the foundations of a new field theory of A. Einstein; (Second part),” Zeit. Phys. 54 (1929), 590-593…………………………………………… 89 (Received on March 4) R. -
Curvature Tensors in a 4D Riemann–Cartan Space: Irreducible Decompositions and Superenergy
Curvature tensors in a 4D Riemann–Cartan space: Irreducible decompositions and superenergy Jens Boos and Friedrich W. Hehl [email protected] [email protected]"oeln.de University of Alberta University of Cologne & University of Missouri (uesday, %ugust 29, 17:0. Geometric Foundations of /ravity in (artu Institute of 0hysics, University of (artu) Estonia Geometric Foundations of /ravity Geometric Foundations of /auge Theory Geometric Foundations of /auge Theory ↔ Gravity The ingredients o$ gauge theory: the e2ample o$ electrodynamics ,3,. The ingredients o$ gauge theory: the e2ample o$ electrodynamics 0henomenological Ma24ell: redundancy conserved e2ternal current 5 ,3,. The ingredients o$ gauge theory: the e2ample o$ electrodynamics 0henomenological Ma24ell: Complex spinor 6eld: redundancy invariance conserved e2ternal current 5 conserved #7,8 current ,3,. The ingredients o$ gauge theory: the e2ample o$ electrodynamics 0henomenological Ma24ell: Complex spinor 6eld: redundancy invariance conserved e2ternal current 5 conserved #7,8 current Complete, gauge-theoretical description: 9 local #7,) invariance ,3,. The ingredients o$ gauge theory: the e2ample o$ electrodynamics 0henomenological Ma24ell: iers Complex spinor 6eld: rce carr ry of fo mic theo rrent rosco rnal cu m pic en exte att desc gredundancyiv er; N ript oet ion o conserved e2ternal current 5 invariance her f curr conserved #7,8 current e n t s Complete, gauge-theoretical description: gauge theory = complete description of matter and 9 local #7,) invariance how it interacts via gauge bosons ,3,. Curvature tensors electrodynamics :ang–Mills theory /eneral Relativity 0oincaré gauge theory *3,. Curvature tensors electrodynamics :ang–Mills theory /eneral Relativity 0oincaré gauge theory *3,. Curvature tensors electrodynamics :ang–Mills theory /eneral Relativity 0oincar; gauge theory *3,. -
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 . -
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. -
Graduate Student Research Day 2010 Florida Atlantic University
Graduate Student Research Day 2010 Florida Atlantic University CHARLES E. SCHMIDT COLLEGE OF SCIENCE Improvements to Moving Puncture Initial Data and Analysis of Gravitational Waveforms using the BSSN Formalism on the BAM Code George Reifenberger Charles E. Schmidt College of Science, Florida Atlantic University Faculty Advisor: Dr. Wolfgang Tichy Numerical relativity has only recently been able to simulate the creation of gravitational wave signatures through techniques concerning both the natural complexities of general relativity and the computational requirements needed to obtain significant accuracies. These gravitational wave signatures will be used as templates for detection. The need to develop better results has divided the field into specific areas of code development, one of which involves improvement on the construction of binary black hole initial data. Gravitational waves are a prediction of general relativity, however none have currently been observed experimentally. The search for gravitational wave signatures from binary black hole mergers has required many sub-disciplines of general relativity to contribute to the effort; numerical relativity being one of these. Assuming speeds much smaller than the speed of light Post-Newtonian approximations are introduced into initial data schemes. Evolution of this initial data using the BSSN formalism has approximately satisfied constraint equations of General Relativity to produce probable gravitational wave signatures. Analysis of data convergence and behavior of physical quantities shows appropriate behavior of the simulation and allows for the wave signatures to be considered for template inclusion. High order convergence of our data validates the accuracy of our code, and the wave signatures produced can be used as an improved foundation for more physical models. -
Status of Numerical Relativity: from My Personal Point of View Masaru Shibata (U
Status of Numerical Relativity: From my personal point of view Masaru Shibata (U. Tokyo) 1 Introduction 2 General issues in numerical relativity 3 Current status of implementation 4 Some of our latest numerical results: NS-NS merger & Stellar core collapse 5 Summary & perspective 1: Introduction: Roles in NR A To predict gravitational waveforms: Two types of gravitational-wave detectors work now or soon. h Space Interferometer Ground Interferometer LISA LIGO/VIRGO/ Physics of GEO/TAMA SMBH BH-BH SMBH/SMBH NS-NS SN Frequency 0.1mHz 0.1Hz 10Hz 1kHz Templates (for compact binaries, core collapse, etc) should be prepared B To simulate Astrophysical Phenomena e.g. Central engine of GRBs = Stellar-mass black hole + disks (Probably) NS-NS merger BH-NS merger ? Best theoretical approach Stellar collapse of = Simulation in GR rapidly rotating star C To discover new phenomena in GR In the past 20 years, community has discovered e.g., 1: Critical phenomena (Choptuik) 2: Toroidal black hole (Shapiro-Teukolsky) 3: Naked singularity formation (Nakamura, S-T) GR phenomena to be simulated ASAP ・ NS-NS / BH-NS /BH-BH mergers (Promising GW sources/GRB) ・ Stellar collapse of massive star to a NS/BH (Promising GW sources/GRB) ・ Nonaxisymmetric dynamical instabilities of rotating NSs (Promising GW sources) ・ …. In general, 3D simulations are necessary 2 Issues: Necessary elements for GR simulations • Einstein’s evolution equations solver • GR Hydrodynamic equations solver • Appropriate gauge conditions (coordinate conditions) • Realistic initial conditions