The Equations of Motion of the Post-Newtonian Compact Binary Inspirals As Gravitational Radiation Sources Under the Effective Field Theory Formalism
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The Levi-Civita Tensor Noncovariance and Curvature in the Pseudotensors
The Levi-Civita tensor noncovariance and curvature in the pseudotensors space A. L. Koshkarov∗ University of Petrozavodsk, Physics department, Russia Abstract It is shown that conventional ”covariant” derivative of the Levi-Civita tensor Eαβµν;ξ is not really covariant. Adding compensative terms, it is possible to make it covariant and to be equal to zero. Then one can be introduced a curvature in the pseudotensors space. There appears a curvature tensor which is dissimilar to ordinary one by covariant term including the Levi-Civita density derivatives hence to be equal to zero. This term is a little bit similar to Weylean one in the Weyl curvature tensor. There has been attempted to find a curvature measure in the combined (tensor plus pseudotensor) tensors space. Besides, there has been constructed some vector from the metric and the Levi-Civita density which gives new opportunities in geometry. 1 Introduction Tensor analysis which General Relativity is based on operates basically with true tensors and it is very little spoken of pseudotensors role. Although there are many objects in the world to be bound up with pseudotensors. For example most of particles and bodies in the Universe have angular momentum or spin. Here is a question: could a curvature tensor be a pseudotensor or include that in some way? It’s not clear. Anyway, symmetries of the Riemann-Christopher tensor are not compatible with those of the Levi-Civita pseudotensor. There are examples of using values in Physics to be a sum of a tensor and arXiv:0906.0647v1 [physics.gen-ph] 3 Jun 2009 a pseudotensor. -
Arxiv:0911.0334V2 [Gr-Qc] 4 Jul 2020
Classical Physics: Spacetime and Fields Nikodem Poplawski Department of Mathematics and Physics, University of New Haven, CT, USA Preface We present a self-contained introduction to the classical theory of spacetime and fields. This expo- sition is based on the most general principles: the principle of general covariance (relativity) and the principle of least action. The order of the exposition is: 1. Spacetime (principle of general covariance and tensors, affine connection, curvature, metric, tetrad and spin connection, Lorentz group, spinors); 2. Fields (principle of least action, action for gravitational field, matter, symmetries and conservation laws, gravitational field equations, spinor fields, electromagnetic field, action for particles). In this order, a particle is a special case of a field existing in spacetime, and classical mechanics can be derived from field theory. I dedicate this book to my Parents: Bo_zennaPop lawska and Janusz Pop lawski. I am also grateful to Chris Cox for inspiring this book. The Laws of Physics are simple, beautiful, and universal. arXiv:0911.0334v2 [gr-qc] 4 Jul 2020 1 Contents 1 Spacetime 5 1.1 Principle of general covariance and tensors . 5 1.1.1 Vectors . 5 1.1.2 Tensors . 6 1.1.3 Densities . 7 1.1.4 Contraction . 7 1.1.5 Kronecker and Levi-Civita symbols . 8 1.1.6 Dual densities . 8 1.1.7 Covariant integrals . 9 1.1.8 Antisymmetric derivatives . 9 1.2 Affine connection . 10 1.2.1 Covariant differentiation of tensors . 10 1.2.2 Parallel transport . 11 1.2.3 Torsion tensor . 11 1.2.4 Covariant differentiation of densities . -
Testing General Relativity Through the Computation of Radiative Terms And
TESTING GENERAL RELATIVITY THROUGH THE COMPUTATION OF RADIATIVE TERMS AND WITHIN THE NEUTRON STAR STRONG-FIELD REGIME by Alexander Saffer A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Physics MONTANA STATE UNIVERSITY Bozeman, Montana April 2019 ©COPYRIGHT by Alexander Saffer 2019 All Rights Reserved ii DEDICATION Dedicated to my family, who provided me with their unconditional love and support. iii ACKNOWLEDGEMENTS I would like to acknowledge the hard work of my advisor Dr. Nicolás Yunes, whose dedication and compassion for physics and those in this field has taught me more than classes ever could. I would also like to thank the Dr. Kent Yagi and Dr. Hector Okada da Silva for their willingness to always help me no matter what I asked and for having the patience to put up with me whenever I struggled. In addition, I would like to thank Dr. Neil Cornish and the rest of the eXtreme Gravity Institute for providing an environment conducive to success. Lastly, I would like to thank my family and friends both within and outside of the MSU physics department who provided their support and guidance over these past 6 years, especially Meg. iv TABLE OF CONTENTS 1. INTRODUCTION ................................................................................................ 1 2. THE GRAVITATIONAL WAVESTRESS-ENERGY (PSEUDO)-TENSOR IN MODIFIED GRAVITY ...................................................................................12 Contribution of Authors and Co-Authors...............................................................12 -
Tensor Calculus and Differential Geometry
Course Notes Tensor Calculus and Differential Geometry 2WAH0 Luc Florack March 10, 2021 Cover illustration: papyrus fragment from Euclid’s Elements of Geometry, Book II [8]. Contents Preface iii Notation 1 1 Prerequisites from Linear Algebra 3 2 Tensor Calculus 7 2.1 Vector Spaces and Bases . .7 2.2 Dual Vector Spaces and Dual Bases . .8 2.3 The Kronecker Tensor . 10 2.4 Inner Products . 11 2.5 Reciprocal Bases . 14 2.6 Bases, Dual Bases, Reciprocal Bases: Mutual Relations . 16 2.7 Examples of Vectors and Covectors . 17 2.8 Tensors . 18 2.8.1 Tensors in all Generality . 18 2.8.2 Tensors Subject to Symmetries . 22 2.8.3 Symmetry and Antisymmetry Preserving Product Operators . 24 2.8.4 Vector Spaces with an Oriented Volume . 31 2.8.5 Tensors on an Inner Product Space . 34 2.8.6 Tensor Transformations . 36 2.8.6.1 “Absolute Tensors” . 37 CONTENTS i 2.8.6.2 “Relative Tensors” . 38 2.8.6.3 “Pseudo Tensors” . 41 2.8.7 Contractions . 43 2.9 The Hodge Star Operator . 43 3 Differential Geometry 47 3.1 Euclidean Space: Cartesian and Curvilinear Coordinates . 47 3.2 Differentiable Manifolds . 48 3.3 Tangent Vectors . 49 3.4 Tangent and Cotangent Bundle . 50 3.5 Exterior Derivative . 51 3.6 Affine Connection . 52 3.7 Lie Derivative . 55 3.8 Torsion . 55 3.9 Levi-Civita Connection . 56 3.10 Geodesics . 57 3.11 Curvature . 58 3.12 Push-Forward and Pull-Back . 59 3.13 Examples . 60 3.13.1 Polar Coordinates in the Euclidean Plane . -
Pseudotensors
Pseudotensors Math 1550 lecture notes, Prof. Anna Vainchtein 1 Proper and improper orthogonal transfor- mations of bases Let {e1, e2, e3} be an orthonormal basis in a Cartesian coordinate system and suppose we switch to another rectangular coordinate system with the orthonormal basis vectors {¯e1, ¯e2, ¯e3}. Recall that the two bases are related via an orthogonal matrix Q with components Qij = ¯ei · ej: ¯ei = Qijej, ei = Qji¯ei. (1) Let ∆ = detQ (2) and recall that ∆ = ±1 because Q is orthogonal. If ∆ = 1, we say that the transformation is proper orthogonal; if ∆ = −1, it is an improper orthogonal transformation. Note that the handedness of the basis remains the same under a proper orthogonal transformation and changes under an improper one. Indeed, ¯ V = (¯e1 ׯe2)·¯e3 = (Q1mem ×Q2nen)·Q3lel = Q1mQ2nQ3l(em ×en)·el, (3) where the cross product is taken with respect to some underlying right- handed system, e.g. standard basis. Note that this is a triple sum over m, n and l. Now, observe that the terms in the above some where (m, n, l) is a cyclic (even) permutation of (1, 2, 3) all multiply V = (e1 × e2) · e3 because the scalar triple product is invariant under such permutations: (e1 × e2) · e3 = (e2 × e3) · e1 = (e3 × e1) · e2. Meanwhile, terms where (m, n, l) is a non-cyclic (odd) permutations of (1, 2, 3) multiply −V , e.g. for (m, n, l) = (2, 1, 3) we have (e2 × e1) · e3 = −(e1 × e2) · e3 = −V . All other terms in the sum in (3) (where two or more of the three indices (m, n, l) are the same) are zero (why?). -
Benjamin J. Owen - Curriculum Vitae
BENJAMIN J. OWEN - CURRICULUM VITAE Contact information Mail: Texas Tech University Department of Physics & Astronomy Lubbock, TX 79409-1051, USA E-mail: [email protected] Phone: +1-806-834-0231 Fax: +1-806-742-1182 Education 1998 Ph.D. in Physics, California Institute of Technology Thesis title: Gravitational waves from compact objects Thesis advisor: Kip S. Thorne 1993 B.S. in Physics, magna cum laude, Sonoma State University (California) Minors: Astronomy, German Research advisors: Lynn R. Cominsky, Gordon G. Spear Academic positions Primary: 2015{ Professor of Physics & Astronomy Texas Tech University 2013{2015 Professor of Physics The Pennsylvania State University 2008{2013 Associate Professor of Physics The Pennsylvania State University 2002{2008 Assistant Professor of Physics The Pennsylvania State University 2000{2002 Research Associate University of Wisconsin-Milwaukee 1998{2000 Research Scholar Max Planck Institute for Gravitational Physics (Golm) Secondary: 2015{2018 Adjunct Professor The Pennsylvania State University 2012 (2 months) Visiting Scientist Max Planck Institute for Gravitational Physics (Hanover) 2010 (6 months) Visiting Associate LIGO Laboratory, California Institute of Technology 2009 (6 months) Visiting Scientist Max Planck Institute for Gravitational Physics (Hanover) Honors and awards 2017 Princess of Asturias Award for Technical and Scientific Research (with the LIGO Scientific Collaboration) 2017 Albert Einstein Medal (with the LIGO Scientific Collaboration) 2017 Bruno Rossi Prize for High Energy Astrophysics (with the LIGO Scientific Collaboration) 2017 Royal Astronomical Society Group Achievement Award (with the LIGO Scientific Collab- oration) 2016 Gruber Cosmology Prize (with the LIGO Scientific Collaboration) 2016 Special Breakthrough Prize in Fundamental Physics (with the LIGO Scientific Collabora- tion) 2013 Fellow of the American Physical Society 1998 Milton and Francis Clauser Prize for Ph.D. -
Energy-Momentum Pseudotensor and Superpotential for Generally
Energy-momentum pseudotensor and superpotential for generally covariant theories of gravity of general form R. V. Ilin,∗ S. A. Paston† Saint Petersburg State University, Saint Petersburg, Russia Abstract The current paper is devoted to the investigation of the general form of the energy- momentum pseudotensor (pEMT) and the corresponding superpotential for the wide class of theories. The only requirement for such a theory is the general covariance of the action without any restrictions on the order of derivatives of the independent variables in it or their transformation laws. As a result of the generalized Noether procedure, we obtain a recurrent chain of the equations, which allows one to express canonical pEMT as a divergence of the superpotential. The explicit expression for this superpotential is also given. We discuss the structure of the obtained expressions and the conditions for the derived pEMT conservation laws to be satisfied independently (fully or partially) of the equations of motion. Deformations of the superpotential form for theories with a change of the independent variables in the action are also considered. We apply these results to some interesting particular cases: General Relativity and its modifications, particularly mimetic gravity and Regge-Teitelboim embedding gravity. arXiv:2010.07073v1 [gr-qc] 14 Oct 2020 ∗E-mail: [email protected] †E-mail: [email protected] 1 1 Introduction One of the traditional issues of General Relativity (GR) is the correct definition of the conserved quantities related to the space-time symmetries, especially the energy. This problem is not special for GR and in general remains for all generally covariant theories. -
AAS Newsletter (ISSN 8750-9350) Is Amateur
AASAAS NNEWSLETTEREWSLETTER March 2003 A Publication for the members of the American Astronomical Society Issue 114 President’s Column Caty Pilachowski, [email protected] Inside The State of the AAS Steve Maran, the Society’s Press Officer, describes the January meeting of the AAS as “the Superbowl 2 of astronomy,” and he is right. The Society’s Seattle meeting, highlighted in this issue of the Russell Lecturer Newsletter, was a huge success. Not only was the venue, the Reber Dies Washington State Convention and Trade Center, spectacular, with ample room for all of our activities, exhibits, and 2000+ attendees at Mt. Stromlo Observatory 3 Bush fires in and around the Council Actions the stimulating lectures in plenary sessions, but the weather was Australian Capital Territory spectacular as well. It was a meeting packed full of exciting science, have destroyed much of the 3 and those of us attending the meeting struggled to attend as many Mt. Stromlo Observatory. Up- Election Results talks and see as many posters as we could. Many, many people to-date information on the stopped me to say what a great meeting it was. The Vice Presidents damage and how the US 4 and the Executive Office staff, particularly Diana Alexander, deserve astronomy community can Astronomical thanks from us all for putting the Seattle meeting together. help is available at Journal www.aas.org/policy/ Editor to Retire Our well-attended and exciting meetings are just one manifestation stromlo.htm. The AAS sends its condolences to our of the vitality of the AAS. Worldwide, our Society is viewed as 8 Australian colleagues and Division News strong and vigorous, and other astronomical societies look to us as stands ready to help as best a model for success. -
Measuring the Black Hole Spin Direction in 3D Cartesian Numerical Relativity Simulations
Measuring the black hole spin direction in 3D Cartesian numerical relativity simulations Vassilios Mewes,1 Jos´eA. Font,1, 2 and Pedro J. Montero3 1Departamento de Astronom´ıa y Astrof´ısica, Universitat de Val`encia, Dr. Moliner 50, 46100, Burjassot (Val`encia), Spain 2Observatori Astron`omic, Universitat de Val`encia, C/ Catedr´atico Jos´eBeltr´an 2, 46980, Paterna (Val`encia), Spain 3Max-Planck-Institute f¨ur Astrophysik, Karl-Schwarzschild-Str. 1, 85748, Garching bei M¨unchen, Germany We show that the so-called flat-space rotational Killing vector method for measuring the Cartesian components of a black hole spin can be derived from the surface integral of Weinberg’s pseudoten- sor over the apparent horizon surface when using Gaussian normal coordinates in the integration. Moreover, the integration of the pseudotensor in this gauge yields the Komar angular momentum integral in a foliation adapted to the axisymmetry of the spacetime. As a result, the method does not explicitly depend on the evolved lapse α and shift βi on the respective timeslice, as they are fixed to Gaussian normal coordinates, while leaving the coordinate labels of the spatial metric γij and the extrinsic curvature Kij unchanged. Such gauge fixing endows the method with coordi- nate invariance, which is not present in integral expressions using Weinberg’s pseudotensor, as they normally rely on the explicit use of Cartesian coordinates. PACS numbers: 04.25.Dm, 95.30.Sf, 97.60.Lf I. INTRODUCTION surface integral on the apparent horizon (AH) of the BH 1 a b JAH = ψ R Kab dS, (1) Since the binary black hole (BBH) merger break- 8π ZS through simulations of about a decade ago [1–3], ever- a growing computational resources and advances in the where ψ is an approximate rotational Killing vector on numerical methods used to simulate these systems have the horizon that has to be determined numerically (see a b made the exploration of the vast initial parameter space [8] for a method of finding ψ ), R is the outward point- possible (see e.g. -
Curriculum Vitae
Curriculum Vitae Luis R. Lehner April 2020 1 Personal Data: Name and Surname: Luis R. LEHNER Marital Status: Married Date of Birth: July 17th. 1970 Current Address: Perimeter Institute for Theoretical Physics, 31 Caroline St. N. Waterloo, ON, N2L 2Y5 Canada Tel.: 519) 569-7600 Ext 6571 Mail Address: [email protected] Fax: (519) 569-7611 2 Education: • Ph.D. in Physics; University of Pittsburgh; 1998. Title: Gravitational Radiation from Black Hole spacetimes. Advisor: Jeffrey Winicour, PhD. • Licenciado en F´ısica;FaMAF, Universidad Nacional de C´ordoba;1993. Title: On a Simple Model for Compact Objects in General Relativity. Advisor: Osvaldo M. Moreschi, PhD. 3 Awards, Honors & Fellowships • \TD's 10 most influential Hispanic Canadian" 2019. • \Resident Theorist" for the Gravitational Wave International Committee 2018-present. • Member of the Advisory Board of the Kavli Institute for Theoretical Physics (UCSB) 2016-2020. • Executive Committee Member of the CIFAR programme: \Gravity and the Extreme Universe" 2017-present. • Member of the Scientific Council of the ICTP South American Institute for Fundamental Research (ICTP- SAIFR) 2015-present. • Fellow International Society of General Relativity and Gravitation, 2013-. • Discovery Accelerator Award, NSERC, Canada 2011-2014. • American Physical Society Fellow 2009-. • Canadian Institute for Advanced Research Fellow 2009-. 1 • Kavli-National Academy of Sciences Fellow 2008, 2017. • Louisiana State University Rainmaker 2008. • Baton Rouge Business Report Top 40 Under 40. 2007. • Scientific Board Member of Teragrid-NSF. 2006-2009. • Institute of Physics Fellow. The Institute of Physics, UK, 2004 -. • Phi Kappa Phi Non-Tenured Faculty Award in Natural and Physical Sciences. Louisiana State University, 2004. • Canadian Institute for Advanced Research Associate Member, 2004 -. -
A Gentle Introduction to Tensors (2014)
A Gentle Introduction to Tensors Boaz Porat Department of Electrical Engineering Technion – Israel Institute of Technology [email protected] May 27, 2014 Opening Remarks This document was written for the benefits of Engineering students, Elec- trical Engineering students in particular, who are curious about physics and would like to know more about it, whether from sheer intellectual desire or because one’s awareness that physics is the key to our understanding of the world around us. Of course, anybody who is interested and has some college background may find this material useful. In the future, I hope to write more documents of the same kind. I chose tensors as a first topic for two reasons. First, tensors appear everywhere in physics, including classi- cal mechanics, relativistic mechanics, electrodynamics, particle physics, and more. Second, tensor theory, at the most elementary level, requires only linear algebra and some calculus as prerequisites. Proceeding a small step further, tensor theory requires background in multivariate calculus. For a deeper understanding, knowledge of manifolds and some point-set topology is required. Accordingly, we divide the material into three chapters. The first chapter discusses constant tensors and constant linear transformations. Tensors and transformations are inseparable. To put it succinctly, tensors are geometrical objects over vector spaces, whose coordinates obey certain laws of transformation under change of basis. Vectors are simple and well-known examples of tensors, but there is much more to tensor theory than vectors. The second chapter discusses tensor fields and curvilinear coordinates. It is this chapter that provides the foundations for tensor applications in physics. -
The Poor Man's Introduction to Tensors
The Poor Man’s Introduction to Tensors Justin C. Feng Preface In the spring semester of 2013, I took a graduate fluid mechanics class taught by Philip J. Morrison. On thefirst homework assignment, I found that it was easier to solve some of the problems using tensors in the coordinate basis, but I was uncomfortable with it because I wasn’t sure if I was allowed to use a formalism that had not been taught in class. Eventually, I decided that if I wrote an appendix on tensors, I would be allowed to use the formalism. Sometime in 2014, I converted1 the appendix into a set of introductory notes on tensors and posted it on my academic website, figuring that they might be useful for someone interested in learning thetopic. Over the past three years, I had become increasingly dissatisfied with the notes. The biggest issue with these notes was that they were typeset in Mathematica—during my early graduate career, I typeset my homework assignments in Mathematica, and it was easiest to copy and paste the appendix into another Mathematica notebook (Mathematica does have a feature to convert notebooks to TeX, but much of the formatting is lost in the process). I had also become extremely dissatisfied with the content—the notes contained many formulas that weren’t sufficiently justified, and there were many examples of sloppy reasoning throughout. At one point, I had even considered removing the notes from my website, but after receiving some positive feedback from students who benefited from the notes, I decided to leave it up for the time being, vowing to someday update and rewrite these notes in TeX.