Beyond the Einstein Addition Law and Its Gyroscopic Thomas Precession Fundamental Theories of Physics
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Thomas Precession and Thomas-Wigner Rotation: Correct Solutions and Their Implications
epl draft Header will be provided by the publisher This is a pre-print of an article published in Europhysics Letters 129 (2020) 3006 The final authenticated version is available online at: https://iopscience.iop.org/article/10.1209/0295-5075/129/30006 Thomas precession and Thomas-Wigner rotation: correct solutions and their implications 1(a) 2 3 4 ALEXANDER KHOLMETSKII , OLEG MISSEVITCH , TOLGA YARMAN , METIN ARIK 1 Department of Physics, Belarusian State University – Nezavisimosti Avenue 4, 220030, Minsk, Belarus 2 Research Institute for Nuclear Problems, Belarusian State University –Bobrujskaya str., 11, 220030, Minsk, Belarus 3 Okan University, Akfirat, Istanbul, Turkey 4 Bogazici University, Istanbul, Turkey received and accepted dates provided by the publisher other relevant dates provided by the publisher PACS 03.30.+p – Special relativity Abstract – We address to the Thomas precession for the hydrogenlike atom and point out that in the derivation of this effect in the semi-classical approach, two different successions of rotation-free Lorentz transformations between the laboratory frame K and the proper electron’s frames, Ke(t) and Ke(t+dt), separated by the time interval dt, were used by different authors. We further show that the succession of Lorentz transformations KKe(t)Ke(t+dt) leads to relativistically non-adequate results in the frame Ke(t) with respect to the rotational frequency of the electron spin, and thus an alternative succession of transformations KKe(t), KKe(t+dt) must be applied. From the physical viewpoint this means the validity of the introduced “tracking rule”, when the rotation-free Lorentz transformation, being realized between the frame of observation K and the frame K(t) co-moving with a tracking object at the time moment t, remains in force at any future time moments, too. -
Finslerian Geometries Fundamental Theories of Physics
Finslerian Geometries Fundamental Theories of Physics An International Book Series on The Fundamental Theories of Physics: Their Clarification, Development and Application Editor: ALWYN VAN DER MERWE, University of Denver, U.S.A. Editorial Advisory Board: LAWRENCE P. HORWITZ, Tel-Aviv University, Israel BRIAN D. JOSEPHSON, University of Cambridge, u.K. CLIVE KILMISTER, University of London, U.K. PEKKA J. LAHTI, University of Turku, Finland GUNTER LUDWIG, Philipps-Universitiit, Marburg, Germany NATHAN ROSEN, Israel Institute of Technology, Israel ASHER PERES, Israel Institute of Technology, Israel EDUARD PRUGOVECKI, University of Toronto, Canada MENDEL SACHS, State University of New York at Buffalo, U.S.A. ABDUS SALAM, International Centre for Theoretical Physics, Trieste, Italy HANS-JURGEN TREDER, Zentralinstitut fur Astrophysik der Akademie der Wissenschaften, Germany Volume 109 Finslerian Geometries A Meeting of Minds edited by P.L. Antonell i DeJXlrlmem of Mathematical Sciences, University ofAlberta, EdmonlOn. Alberta, Canada SPRINGER-SCIENCE+BUSINESS MEDIA, B.V. A C .I.P. Catalogue record for this book is available from the Library of Congress. ISBN 978-94-010-5838-4 ISBN 978-94-011-4235-9 (eBook) DOI 10.1007/978-94-011-4235-9 Printed an arid1ree paper AH Rights Reserved © 2000 Springer Science+Business Media Dordrecht Originally published by K!uwer Academic Publishers in 2000 Soticovcr repri Il! of the hardcover l s( cd ition in 20()(} No part of the material protected by this copyright natice may be reproduced Of utilized in any farm Of by any means, electronic or mechanical, induding pholocopying, recording or by any informat ion slorage and relrieval system, withoUI wrinen permissian from the copyright owner. -
Covariant Calculation of General Relativistic Effects in an Orbiting Gyroscope Experiment
PHYSICAL REVIEW D 67, 062003 ͑2003͒ Covariant calculation of general relativistic effects in an orbiting gyroscope experiment Clifford M. Will* McDonnell Center for the Space Sciences, Department of Physics, Washington University, St. Louis, Missouri 63130 ͑Received 17 December 2002; published 26 March 2003͒ We carry out a covariant calculation of the measurable relativistic effects in an orbiting gyroscope experi- ment. The experiment, currently known as Gravity Probe B, compares the spin directions of an array of spinning gyroscopes with the optical axis of a telescope, all housed in a spacecraft that rolls about the optical axis. The spacecraft is steered so that the telescope always points toward a known guide star. We calculate the variation in the spin directions relative to readout loops rigidly fixed in the spacecraft, and express the variations in terms of quantities that can be measured, to sufficient accuracy, using an Earth-centered coordi- nate system. The measurable effects include the aberration of starlight, the geodetic precession caused by space curvature, the frame-dragging effect caused by the rotation of the Earth and the deflection of light by the Sun. DOI: 10.1103/PhysRevD.67.062003 PACS number͑s͒: 04.80.Cc I. INTRODUCTION by the on-board telescope, which is to be trained on a star IM Pegasus ͑HR 8703͒ in our galaxy. One important feature of Gravity Probe B—the ‘‘gyroscope experiment’’—is a this star is that it is also a strong radio source, so that its NASA space experiment designed to measure the general direction and proper motion relative to the larger system of relativistic effect known as the dragging of inertial frames. -
Generalized Gyrovector Spaces and the Positive Cone of a Unital C
Generalized gyrovector spaces and the positive cone of Contact Information: ∗ Faculty of Engineering a unital C -algebra Niigata University 8050 2no-cho ikarashi Nishi-ku Niigata-shi, Niigata- ken, Japan Toshikazu Abe Phone: +81 (25) 262 7469 Niigata University, Faculty of Engineering Email: [email protected] Abstract Definition 1. A magma (G; ⊕) is called a gyrogroup if there exists an Note that a real normed space (V; +; ×) is a GGV with ϕ = idV. Results The concept of generalized gyrovecor space (GGV, for short) is a com- element e such that the binary operation ⊕ satisfies the following (G1) On a GGV, we can define the gyromidpoint. It is a algebraic mid- mon generalization of the concept of real normed spaces and of the gyrovector spaces. The addition of a GGV is not necessarily a commutative group but is a to (G5). point on the GGV. On a real normed space, the gyromidpoint is the A Mazur-Ulam Theorem for GGV’s gyrocommutative gyrogroup. A typical example of GGV’s is the positive cone 8 2 ⊕ arithmetric mean. ∗ (G1) a G, e a = a. of a unital C -algebra. (G; ⊕; ⊗) p(a; b) We have a Mazur-Ulam type theorem for GGV’s as follows. This is a (G2) 8a 2 G, 9 ⊖ a s.t. ⊖a ⊕ a = e: Definition 4. Let be a GGV. The gyromidpoint of a; b 2 (G; ⊕; ⊗) is defined as p(a; b) = 1 ⊗ (a ⊞ b), where ⊞ is the generalization of the celebrated Mazur-Ulam theorem. A proof of this 8 2 9 2 ⊕ ⊕ ⊕ ⊕ 2 (G3) a; b; c G, ! gyr[a; b]c G s.t. -
Thomas Precession Is the Basis for the Structure of Matter and Space Preston Guynn
Thomas Precession is the Basis for the Structure of Matter and Space Preston Guynn To cite this version: Preston Guynn. Thomas Precession is the Basis for the Structure of Matter and Space. 2018. hal- 02628032 HAL Id: hal-02628032 https://hal.archives-ouvertes.fr/hal-02628032 Submitted on 26 May 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Thomas Precession is the Basis for the Structure of Matter and Space Einstein's theory of special relativity was incomplete as originally formulated since it did not include the rotational effect described twenty years later by Thomas, now referred to as Thomas precession. Though Thomas precession has been accepted for decades, its relationship to particle structure is a recent discovery, first described in an article titled "Electromagnetic effects and structure of particles due to special relativity". Thomas precession acts as a velocity dependent counter-rotation, so that at a rotation velocity of 3 / 2 c , precession is equal to rotation, resulting in an inertial frame of reference. During the last year and a half significant progress was made in determining further details of the role of Thomas precession in particle structure, fundamental constants, and the galactic rotation velocity. -
From the Lorentz Transformation Group in Pseudo-Euclidean Spaces to Bi-Gyrogroups
Mathematics Interdisciplinary Research 1 (2016) 229 − 272 From the Lorentz Transformation Group in Pseudo-Euclidean Spaces to Bi-Gyrogroups Abraham A. Ungar? Abstract The Lorentz transformation of order (m = 1; n), n 2 N, is the well-known Lorentz transformation of special relativity theory. It is a transformation of m=1;n time-space coordinates of the pseudo-Euclidean space R of one time di- mension and n space dimensions (n = 3 in physical applications). A Lorentz transformation without rotations is called a boost. Commonly, the special relativistic boost is parametrized by a relativistically admissible velocity pa- n n rameter v, v 2 Rc , whose domain is the c-ball Rc of all relativistically n n admissible velocities, Rc = fv 2 R : kvk < cg, where the ambient space n R is the Euclidean n-space, and c > 0 is an arbitrarily fixed positive con- stant that represents the vacuum speed of light. The study of the Lorentz transformation composition law in terms of parameter composition reveals that the group structure of the Lorentz transformation of order (m = 1; n) induces a gyrogroup and a gyrovector space structure that regulate the pa- n rameter space Rc . The gyrogroup and gyrovector space structure of the ball n Rc , in turn, form the algebraic setting for the Beltrami-Klein ball model of n hyperbolic geometry, which underlies the ball Rc . The aim of this article is to extend the study of the Lorentz transformation of order (m; n) from m = 1 and n ≥ 1 to all m; n 2 N, obtaining algebraic structures called a bi-gyrogroup and a bi-gyrovector space. -
A Semiclassical Kinetic Theory of Dirac Particles and Thomas
A Semiclassical Kinetic Theory of Dirac Particles and Thomas Precession Omer¨ F. DAYI and Eda KILINC¸ARSLAN Physics Engineering Department, Faculty of Science and Letters, Istanbul Technical University, TR-34469, Maslak–Istanbul, Turkey1 Kinetic theory of Dirac fermions is studied within the matrix valued differential forms method. It is based on the symplectic form derived by employing the semiclassical wave packet build of the positive energy solutions of the Dirac equation. A satisfactory definition of the distribution matrix elements imposes to work in the basis where the helicity is diagonal which is also needed to attain the massless limit. We show that the kinematic Thomas precession correction can be studied straightforwardly within this approach. It contributes on an equal footing with the Berry gauge fields. In fact in equations of motion it eliminates the terms arising from the Berry gauge fields. 1 Introduction Dirac equation which describes massive spin-1/2 particles possesses either positive or negative energy solutions described by 4-dimensional spinors. However, to furnish a well defined one particle inter- pretation, instead of employing both type of solutions, a wave packet build of only positive energy plane wave solutions should be preferred. A nonrelativistic semiclassical dynamics can be obtained employing this wave packet. Semiclassical limit may be useful to have a better understanding of some quantum mechanical phenomena. In the massless limit Dirac equation leads to two copies of Weyl arXiv:1508.00781v1 [hep-th] 4 Aug 2015 particles which possess opposite chirality. Recently, the chiral semiclassical kinetic theory has been formulated to embrace the anomalies due to the external electromagnetic fields in 3 + 1 dimensions [1, 2]. -
Can Croatia Join Europe As Competitive Knowledge-Based Society by 2010?
Editorial Can Croatia Join Europe as Competitive Knowledge-based Society by 2010? Mladen Petrovečki1, Vladimir Paar2, Dragan Primorac1 1Ministry of Science, The 21st century has brought important changes in the paradigms of eco- Education and Sports of the nomic development, one of them being a shift toward recognizing knowl- Republic of Croatia, Zagreb, Croatia edge and information as the most important factors of today. The European 2Croatian Academy of Union (EU) has been working hard to become the most competitive knowl- Sciences and Arts, edge-based society in the world, and Croatia, an EU candidate country, has Zagreb, Croatia been faced with a similar task. To establish itself as one of the best knowl- edge-based country in the Eastern European region over the next four years, Croatia realized it has to create an education and science system correspon- dent with European standards and sensitive to labor market needs. For that purpose, the Croatian Ministry of Science, Education, and Sports (MSES) has created and started implementing a complex strategy, consisting of the following key components: the reform of education system in accordance with the Bologna Declaration; stimulation of scientific production by sup- porting national and international research projects; reversing the “brain drain” into “brain gain” and strengthening the links between science and technology; and informatization of the whole education and science sys- tem. In this comprehensive report, we describe the implementation of these > Correspondence to: measures, whose coordination with the EU goals presents a challenge, as well as an opportunity for Croatia to become a knowledge-based society Mladen Petrovečki Assistant Minister for Science by 2010. -
Physical Holonomy, Thomas Precession, and Clifford Algebra
hXWWM UWThPh 1988-39 Physical Holonomy, Thomas Precession, and Clifford Algebra H. Urbantke Institut für Theoretische Physik Universität Wien Abstract After a general discussion of the physical significance of holonomy group transfor mations, a relation between the transports of Fermi-Walker and Levi-Civitä in Special Relativity is pointed out. A well-known example - the Thomas-Wigner angle - is red- erived in a completely frame-independent manner using Clifford algebra. 1 Introduction — Holonomy Groups in Physics Quantum Holonomy has become a rather popular concept in recent /ears, in particular through the work [1] of Berry and Simon; but it is clear that the Aharanov-Bohm effect [2] is a much earlier instance of it. The point is that here the differential geometric idea of parallel transport defined by connections in fibre bundles [3] attains rather direct physical meaning susceptible to experimentation. This is remarkable because parallel transport has been around in differential geometry since 1917, and differential geometry has invaded theoretical physics since the early days of General Relativity, with new impulses coming from Hamiltonian dynamics and gauge theory: yet the significance of connections used to be formal, the 'transformation properties' standing in the forefront, as one can see from the old 'Ricci-Calculus' as used by Einstein and Grossmann [4] or from the way non- abelian gauge fields were introduced by Yang and Mills [5]. The rather indirect 'physical' realization of parallel transport in General Relativity by Schild's 'ladder construction' [6] also stresses this fact; in non-abelian gauge theory I am aware of no physical realization at all. -
Introduction to Soliton Theory: Applications to Mechanics Fundamental Theories of Physics
Introduction to Soliton Theory: Applications to Mechanics Fundamental Theories of Physics An International Book Series on The Fundamental Theories of Physics: Their Clarification, Development and Application Editor: ALWYN VAN DER MERWE, University of Denver, U.S.A. Editorial Advisory Board: GIANCARLO GHIRARDI, University of Trieste, Italy LAWRENCE P. HORWITZ, Tel-Aviv University, Israel BRIAN D. JOSEPHSON, University of Cambridge, U.K. CLIVE KILMISTER, University of London, U.K. PEKKA J. LAHTI, University of Turku, Finland ASHER PERES, Israel Institute of Technology, Israel EDUARD PRUGOVECKI, University of Toronto, Canada FRANCO SELLERI, Università di Bara, Italy TONY SUDBURY, University of York, U.K. HANS-JÜRGEN TREDER, Zentralinstitut für Astrophysik der Akademie der Wissenschaften, Germany Volume 143 Introduction to Soliton Theory: Applications to Mechanics by Ligia Munteanu Institute of Solid Mechanics, Romanian Academy, Bucharest, Romania and Stefania Donescu Technical University of Civil Engineering, Department of Mathematics, Bucharest, Romania KLUWER ACADEMIC PUBLISHERS NEW YORK, BOSTON, DORDRECHT, LONDON, MOSCOW eBook ISBN: 1-4020-2577-7 Print ISBN: 1-4020-2576-9 ©2005 Springer Science + Business Media, Inc. Print ©2004 Kluwer Academic Publishers Dordrecht All rights reserved No part of this eBook may be reproduced or transmitted in any form or by any means, electronic, mechanical, recording, or otherwise, without written consent from the Publisher Created in the United States of America Visit Springer's eBookstore at: http://ebooks.kluweronline.com and the Springer Global Website Online at: http://www.springeronline.com Contents Preface ix Part 1. INTRODUCTION TO SOLITON THEORY 1. MATHEMATICAL METHODS 1 1.1 Scope of the chapter 1 1.2 Scattering theory 1 1.3 Inverse scattering theory 12 1.4 Cnoidal method 17 1.5 Hirota method 25 1.6 Linear equivalence method (LEM) 31 1.7 Bäcklund transformation 39 1.8 Painlevé analysis 46 2. -
Relativity in Rotating Frames Fundamental Theories of Physics
Relativity in Rotating Frames Fundamental Theories of Physics An International Book Series on The Fundamental Theories of Physics: Their Clarification, Development and Application Editor: ALWYN VAN DER MERWE, University of Denver, U.S.A. Editorial Advisory Board: JAMES T. CUSHING, University of Notre Dame, U.S.A. GIANCARLO GHIRARDI, University of Trieste, Italy LAWRENCE P. HORWITZ, Tel-Aviv University, Israel BRIAN D. JOSEPHSON, University of Cambridge, U.K. CLIVE KILMISTER, University of London, U.K. PEKKA J. LAHTI, University of Turku, Finland ASHER PERES, Israel Institute of Technology, Israel EDUARD PRUGOVECKI, University of Toronto, Canada TONY SUDBURY, University of York, U.K. HANS-JÜRGEN TREDER, Zentralinstitut für Astrophysik der Akademie der Wissenschaften, Germany Volume 135 Relativity in Rotating Frames Relativistic Physics in Rotating Reference Frames Edited by Guido Rizzi Politecnico di Torino and Istituto Nazionale di Fisica Nucleare, Torino, Italy and Matteo Luca Ruggiero Politecnico di Torino and Istituto Nazionale di Fisica Nucleare, Torino, Italy SPRINGER-SCIENCE+BUSINESS MEDIA, B.V. A C.I.P. Catalogue record for this book is available from the Library of Congress. ISBN 978-90-481-6514-8 ISBN 978-94-017-0528-8 (eBook) DOI 10.1007/978-94-017-0528-8 Printed on acid-free paper All Rights Reserved © 2004 Springer Science+Business Media Dordrecht Originally published by Kluwer Academic Publishers in 2004 No part of this work may be reproduced, stored in a retrieval system, or transmitted in any form or by any means, electronic, mechanical, photocopying, microfilming, recording or otherwise, without written permission from the Publisher, with the exception of any material supplied specifically for the purpose of being entered and executed on a computer system, for exclusive use by the purchaser of the work. -
Physics 209 Fall 2002 Notes 5 Thomas Precession Jackson's
Physics 209 Fall 2002 Notes 5 Thomas Precession Jackson's discussion of Thomas precession is based on Thomas's original treatment, and on the later paper by Bargmann, Michel, and Telegdi. The alternative treatment presented in these notes is more geometrical in spirit and makes greater effort to identify the aspects of the problem that are dependent on the state of the observer and those that are Lorentz and gauge invariant. There is one part of the problem that involves some algebra (the calculation of Thomas's angular velocity), and this is precisely the part that is dependent on the state of the observer (the calculation is specific to a particular Lorentz frame). The rest of the theory is actually quite simple. In the following we will choose units so that c = 1, except that the c's will be restored in some final formulas. xµ(τ) u e1 e2 e3 u `0 e3 e1 `1 e2 `2 `3 µ Fig. 5.1. Lab frame f`αg and conventional rest frames feαg along the world line x (τ) of a particle. The time-like basis vector e0 of the conventional rest frame is the same as the world velocity u of the particle. The spatial axes of the conventional rest frame fei; i = 1; 2; 3g span the three-dimensional space-like hyperplane orthogonal to the world line. To begin we must be careful of the phrase \the rest frame of the particle," which is used frequently in relativity theory and in the theory of Thomas precession. The geometrical situation is indicated schematically in Fig.