Relativistic Investigations of Laser-Plasma Interactions and Electrodynamics in a Medium.”

Total Page:16

File Type:pdf, Size:1020Kb

Load more

“Relativistic Investigations of Laser-Plasma Interactions and Electrodynamics in a Medium.” by Terrence Pryce Rowlands A thesis submitted for the degree of Doctor of Philosophy at the University of New South Wales Sydney, October 1996 U N S W 1 9 JUM 1997 LIBRARY Statement of Originality I hereby declare that this submission is my own work and that, to the best of my knowledge and belief, it contains no material previously published or written by another person nor material which to a substantial extent has been accepted for the award of any other degree or diploma of a university or other institute of higher learning, except where due acknowledgment is made in the text. I also declare that the intellectual content of this thesis is the product of my own work, even though I may have received assistance from others on style, presentation and language expression. Terrence P. Rowlands B.Sc.(Hons) Sydney, October 1996. page -ii- Acknowledgments I am indebted to Professor H. Hora for suggesting the initial research topic. I am especially grateful to him for maintaining his enthusiasm and assistance after his retirement. I would also like to thank Associate Professor R. Stening for taking over the mantle of supervision after Professor Hora’s retirement. I am indebted to the late Associate Professor (retired) S. Prokhovnik for his mathematical and relativistic insights. Several individuals at the University of New South Wales were very helpful; Dr. John D’Ambra, Associate Professor M. O’Connor, Mrs. M. Ackerman, and others who have provided encouragement and support. Lastly, I would like to extend my gratitude to my family and friends for their understanding during this thesis. In particular I would like to express my unbounded gratitude toward Miss T. Evans. Without her encouragement, support and selflessness, this thesis would never have come to fruition. page -iii- Dedication This thesis is dedicated to the memory of Associate Professor (retired) Simon Prokhovnik whose insight, experience and encouragement was invaluable. page -iv- Abstract The interaction of electromagnetic radiation with plasmas and other media is studied in a relativistic four-vector formalism. A gauge and Lorentz invariant ponderomotive four-force is derived from the time-dependent nonlinear three-force of H. Hora (Phys. Fluids, 12, 182 [1985] ). This four-force, due to it’s Lorentz invariance, contains new magnetic field terms. It is shown to have a symmetric stress-energy tensor. A new gauge and Lorentz invariant model of the response of a plasma to electromagnetic radiation is then devised. An expression for the dispersion relation is obtained from this model. It is then proved that the magnetic permeability of a plasma is unity for a general reference frame. This is an important result since it has been previously assumed in many plasma models. Gauge and Lorentz invariant electrodynamics in a medium is investigated utilizing fourth rank tensors and a redefinition of the Minkowski six-vectors. Initially a general isotropic medium is investigated. The permeability and permittivity are encapsulated within a fourth rank ‘media’ tensor. The fundamental electromagnetic relations are concisely expressed within this fourth rank tensor framework. The refractive index is recovered as an invariant of the fourth rank media tensor. page -v- The generalization of the fourth rank tensor model to encompass anisotropic media is achieved by associating a direction with each tensor component. The fourth rank tensorial relations developed for isotropic media are still valid. The refractive index expression appropriate for the anisotropic medium is then recovered. page -vi- Table of Contents Chapter 1. Introduction........................................................................................... 1 1.1 Overview............................................................................................................ 1 1.2 Introductory Concepts....................................................................................... 3 1.3 Chapter Synopsis............................................................................................... 9 1.3.1 Plasma Response to Electromagnetic Radiation......................................... 9 1.3.2 A Formulation of Electromagnetics in the General Medium.................... 10 1.4 Units and Conventions............................................................... 11 1.5 Bibliography.....................................................................................................12 Chapter 2. Stress-Energy Tensors and Nonlinear Plasma Theory..................... 14 2.1 Introduction......................................................................................................14 2.2 The Abraham-Minkowski Problem...................................................................15 2.2.1 Introduction...............................................................................................15 2.2.2 Asymmetric Stress-Energy Tensors.......................................................... 17 2.2.3 Canonical Stress-Energy Tensors............................................................. 22 2.2.4 More on the Abraham and Minkowski Stress Tensors.............................24 2.3 Plasma Theory and Ponderomotive Forces......................................................26 page -vii- ^ 26 2.3.2 The Time-Independent Ponderomotive Force.............................................. 27 2.3.3 The Time-Independent Nonlinear Ponderomotive Force............................ 29 2.4 The Nonlinear Transient Ponderomotive 4-Force............................................... 33 2.4.1 Introduction.......................................................................................................33 2.4.2 Derivation of the Ponderomotive 4-Force and its Stress-Energy Tensor .34 2.4.3 Gauge Invariance of the Ponderomotive 4-Force.........................................37 2.4.4 Lorentz Invariance of the Ponderomotive 4-Force...................................... 38 2.4.5 An Example for a Specific Current................................................................ 38 2.4.6 The Symmetry of the Nonlinear Ponderomotive Stress Energy Tensor ...39 2.4.7 The Trace of the Nonlinear Ponderomotive Stress Energy Tensor...........41 2.4.8 The Time-Independent Nonlinear Ponderomotive 4-Force.........................44 2.5 Discussion.................................................................................................................46 2.6 Bibliography............................................................................................................. 48 Chapter 3. Relativistic Plasma Theory and the Plasma Magnetic Response.... 50 3.1 Introduction...............................................................................................................50 3.2 Relativistic Plasmas and Electromagnetic waves..................................................51 page -viii- 3.2.1 Introduction 51 3.2.2 Constitutive Equation Methods......................................................................52 3.2.3 Boltzmann-Vlasov methods.............................................................................55 3.2.4 Other approaches..............................................................................................58 3.2.5 Overview........................................................................................................... 63 3.3 The Magnetic Response of a Plasma.....................................................................63 3.3.1 Introduction.......................................................................................................63 3.3.2 Theoretical Tokamak investigations..............................................................64 3.3.3 Quantum theory applied to the Magnetic Response.................................... 67 3.3.4 Overview........................................................................................................... 69 3.4 Relativistic derivation of a value for the Magnetic Permeability....................... 70 3.4.1 Introduction.......................................................................................................70 3.4.2 Considerations.................................................................................................. 70 3.4.3 The Lorentz Force Density..............................................................................72 3.4.4 The Charged Fluid Force Density...................................................................73 3.4.5 Equating the Forces.........................................................................................74 3.4.6 The 4-Current Wave Equation.......................................................................75 page -ix- 3.4.7 A solution to the Wave equation. 76 3.4.8 The Dispersion Relation for the 4-Current Wave Equation.......................77 3.4.9 The Electric and Magnetic response of the Charged Fluid.........................77 3.4.10 The derivation of the Magnetic permeability of a Plasma.........................79 3.4.11 A pressure based modification to the model...............................................83 3.5 Discussion.................................................................................................................85 3.6 Bibliography..............................................................................................................86 Chapter 4. Electrodynamics of Relativistic Isotropic Media..............................
Recommended publications
  • Covariant Electrodynamics in Linear Media: Optical Metric

    Covariant Electrodynamics in Linear Media: Optical Metric

    Covariant electrodynamics in linear media: Optical metric Robert T. Thompson∗ Institute of Applied Physics, Karlsruhe Institute of Technology (KIT), 76131 Karlsruhe, Germany While the postulate of covariance of Maxwell’s equations for all inertial observers led Einstein to special relativity, it was the further demand of general covariance – form invariance under general coordinate transformations, including between accelerating frames – that led to general relativity. Several lines of inquiry over the past two decades, notably the development of metamaterial-based transformation optics, has spurred a greater interest in the role of geometry and space-time co- variance for electrodynamics in ponderable media. I develop a generally covariant, coordinate-free framework for electrodynamics in general dielectric media residing in curved background space-times. In particular, I derive a relation for the spatial medium parameters measured by an arbitrary time- like observer. In terms of those medium parameters I derive an explicit expression for the pseudo- Finslerian optical metric of birefringent media and show how it reduces to a pseudo-Riemannian optical metric for nonbirefringent media. This formulation provides a basis for a unified approach to ray and congruence tracing through media in curved space-times that may smoothly vary among positively refracting, negatively refracting, and vacuum. I. INTRODUCTION The standard vectorial representation of Maxwell’s equations ∂B~ B~ =0, E~ + =0, (1a) ∇ · ∇× ∂t ∂D~ D~ = ρ, H~ = ~j, (1b) ∇ · ∇× − ∂t has been the electrodynamics workhorse since it was codified by Heaviside well over a century ago. But this 3-vector representation harbors a hidden assumption: that space-time is Minkowskian. We may forgive Heaviside this trespass, coming 30 years before Einstein’s seminal paper on general relativity, but no description of electrodynamics would be truly complete without incorporating the properties of the underlying space-time in which the fields exist.
  • Generalized Transformation Optics of Linear Materials

    Generalized Transformation Optics of Linear Materials

    Home Search Collections Journals About Contact us My IOPscience Generalized transformation optics of linear materials This article has been downloaded from IOPscience. Please scroll down to see the full text article. 2011 J. Opt. 13 055105 (http://iopscience.iop.org/2040-8986/13/5/055105) View the table of contents for this issue, or go to the journal homepage for more Download details: IP Address: 152.3.193.67 The article was downloaded on 08/04/2011 at 16:57 Please note that terms and conditions apply. IOP PUBLISHING JOURNAL OF OPTICS J. Opt. 13 (2011) 055105 (12pp) doi:10.1088/2040-8978/13/5/055105 Generalized transformation optics of linear materials Robert T Thompson1, Steven A Cummer2 and Jorg¨ Frauendiener1,3 1 Department of Mathematics and Statistics, University of Otago, PO Box 56, Dunedin 9054, New Zealand 2 Department of Electrical and Computer Engineering and Center for Metamaterials and Integrated Plasmonics, Duke University, Durham, NC 27708, USA 3 Centre of Mathematics for Applications, University of Oslo, PO Box 1053, Blindern, NO-0316 Oslo, Norway E-mail: [email protected] Received 4 February 2011, accepted for publication 8 March 2011 Published 7 April 2011 Online at stacks.iop.org/JOpt/13/055105 Abstract We continue the development of a manifestly four-dimensional, completely covariant, approach to transformation optics in linear dielectric materials begun in a previous paper. This approach, which generalizes the Plebanski based approach, is systematically applicable for all transformations and all general linear materials. Importantly, it enables useful applications such as arbitrary relative motion, transformations from arbitrary non-vacuum initial dielectric media, and arbitrary space–times.
  • On Geodesics of Gradient-Index Optical Metrics and the Optical-Mechanical Analogy

    On Geodesics of Gradient-Index Optical Metrics and the Optical-Mechanical Analogy

    On geodesics of gradient-index optical metrics and the optical-mechanical analogy David Delphenich Spring Valley, OH 45370 USA ____ Abstract: The geodesic equations for optical media whose refractive indices have a non-vanishing gradient are developed. It is shown that when those media are optically isotropic, the light paths will be the null geodesics of a spatial metric that is conformally related to the metric on the ambient space. Various aspects of the optical-mechanical analogy are discussed as they relate to the geodesics of conformally-related metrics. Some applications of the concepts of gradient-index optics to general relativity are examined, such as effective indices of refraction for gravitational lensing and Gordon’s optical metrics for optical media that are in a state of relative motion with respect to an observer. The latter topic is approached from the standpoint of pre-metric electromagnetism. Contents Page 1. Introduction………………………………………………………………………………………… 1 2. Geodesics and Fermat’s principle………………………………………………………………….. 3 a. Geodesics. 3 b. Fermat’s principle. 7 3. Geodesics of conformally-related metrics………………………………………………………….. 10 4. Optical-mechanical analogies……………………………………………………………………… 13 a. Jacobi’s prescription. 14 b. Levi-Civita’s conversion. 17 c. “F = ma” optics. 20 d. Hydrodynamical models. 21 5. Gradient-index optics in general relativity…………………………………………………………. 22 a. Gravitational lensing. 22 b. Gordon’s optical metric. 25 6. Conclusions………………………………………………………………………………………… 29 References………………………………………………………………………………………….. 30 1. Introduction. – The path of a light ray in an optical medium is a geodesic of the spatial metric that prevails in that medium. In the most common optical media, those geodesics will be straight lines that typically change directions only at the interface with another medium.
  • GR Constitutive Laws

    GR Constitutive Laws

    On the electromagnetic constitutive laws that are equivalent to spacetime metrics D. H. Delphenich Spring Valley, OH 45370 USA Abstract: The “raising of both indices” in the components of the Minkowski electromagnetic field strength 2-form F to give the components of the electromagnetic excitation bivector field H can be regarded as being equivalent to an electromagnetic constitutive law, as well as being defined by the components of the spacetime metric. This notion is clarified, and the nature of the equivalent dielectric tensors and magnetic permeability tensors that are defined by some common spacetime metrics is discussed. The relationship of the basic construction to effective metrics is discussed, and, in particular, the fact that this effective metric is more general than the Gordon metric. 1. Introduction. – A new approach to classical electromagnetism has been emerging since the work of Kottler, Tamm, Cartan, and van Dantzig in the early Twentieth Century that goes by the name of “pre-metric electromagnetism” ( 1). The origin of the approach is the idea that the only place in which the background metric of spacetime enters into Maxwell’s equations is by way of the Hodge * operator that allows one to define the codifferential δF of the electromagnetic field strength 2-form F. Some of the illusion that Maxwell’s equations depends upon the Lorentzian structure is created by the fact that so many of the formulations of Maxwell’s equations in terms of differential forms never go beyond the limitations of the “classical electromagnetic vacuum,” whose electromagnetic constitutive properties can be summarized by a dielectric constant ε0 and a magnetic permeability constant µ0 .
  • Spin Hall Effects in General Relativity

    Spin Hall Effects in General Relativity

    Dissertation zur Erlangung des akademischen Grades "doctor rerum naturalium" (Dr. rer. nat.) in der Wissenschaftsdisziplin "Mathematik" Spin Hall effects in General Relativity Marius-Adrian Oancea Diese Dissertation wird eingereicht an der Mathematisch-Naturwissenschaftlichen Fakult¨at der Universit¨atPotsdam, sie wurde angefertigt am Max Planck Institut f¨urGravitationsphysik (Albert Einstein Institut) Ort und Tag der Disputation: Universit¨atPotsdam, Raum 02.09.2.22, 30 M¨arz2021 This work is licensed under a Creative Commons License: Attribution 4.0 International. This does not apply to quoted content from other authors. To view a copy of this license visit https://creativecommons.org/licenses/by/4.0/ Hauptbetreuer: apl. Prof. Dr. Lars Andersson Zweitbetreuer: Dr. habil. J´re ´emie Joudioux Mentor: Prof. Dr. Christian Ba¨r Gutachtern: Prof. Dr. Valeri P. Frolov, Prof. Dr. Peter A. Horvathy Published online on the Publication Server of the University of Potsdam: https://doi.org/10.25932/publishup-50229 https://nbn-resolving.org/urn:nbn:de:kobv:517-opus4-502293 Abstract The propagation of test fields, such as electromagnetic, Dirac, or linearized grav- ity, on a fixed spacetime manifold is often studied by using the geometrical optics approximation. In the limit of infinitely high frequencies, the geometrical optics approximation provides a conceptual transition between the test field and an ef- fective point-particle description. The corresponding point-particles, or wave rays, coincide with the geodesics of the underlying spacetime. For most astrophysical ap- plications of interest, such as the observation of celestial bodies, gravitational lens- ing, or the observation of cosmic rays, the geometrical optics approximation and the effective point-particle description represent a satisfactory theoretical model.
  • Arxiv:2003.13452V2 [Physics.Class-Ph]

    Arxiv:2003.13452V2 [Physics.Class-Ph]

    The geometry of induced electromagnetic fields in moving media C. S. Lopez-Monsalvoa, D. Garcia-Pelaezb,c, A. Rubio-Ponceb, R. Escarela-Perezb aConacyt-Universidad Aut´onoma Metropolitana Azcapotzalco Avenida San Pablo Xalpa 180, Azcapotzalco, Reynosa Tamaulipas, 02200 Ciudad de M´exico, M´exico bUniversidad Aut´onoma Metropolitana Azcapotzalco Avenida San Pablo Xalpa 180, Azcapotzalco, Reynosa Tamaulipas, 02200 Ciudad de M´exico, M´exico cUniversidad Panamericana, Tecoyotitla 366. Col. Ex Hacienda Guadalupe Chimalistac, C.P. 01050 Ciudad de Mexico, Mexico Abstract In this manuscript we provide a fully geometric formulation for the induced electromagnetic fields and their corresponding constitutive relations in moving media. To this end, we present the reader with a brief geometric summary to show how vector calculus electromagnetic theory is embedded in the more general language of differential forms. Then, we consider the class of metric constitutive relations describing the medium in which electromagnetic fields propagate. We explicitly obtain the components of the induced fields in a moving medium, as seen in the the lab rest frame. This allows us to read the expressions for the permitivity, permeability and magnetoelectric matrices for the moving medium which, in turn, can be interpreted as a different physical material from the lab point of view. Keywords: Electromagnetism, Riemannian geometry, Magnetoelectric effect 1. Introduction It has been since the early days of General Relativity that we have seen that the “influence of matter on electromagnetic phenomena is equivalent to the influence of a gravitational field” [1, 2]. That is, in the same manner light rays obey Fermat’s principle while propagating across media, in General Relativity light follows null geodesics on a curved spacetime.