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Dirac Equation - Wikipedia
Dirac equation - Wikipedia https://en.wikipedia.org/wiki/Dirac_equation Dirac equation From Wikipedia, the free encyclopedia In particle physics, the Dirac equation is a relativistic wave equation derived by British physicist Paul Dirac in 1928. In its free form, or including electromagnetic interactions, it 1 describes all spin-2 massive particles such as electrons and quarks for which parity is a symmetry. It is consistent with both the principles of quantum mechanics and the theory of special relativity,[1] and was the first theory to account fully for special relativity in the context of quantum mechanics. It was validated by accounting for the fine details of the hydrogen spectrum in a completely rigorous way. The equation also implied the existence of a new form of matter, antimatter, previously unsuspected and unobserved and which was experimentally confirmed several years later. It also provided a theoretical justification for the introduction of several component wave functions in Pauli's phenomenological theory of spin; the wave functions in the Dirac theory are vectors of four complex numbers (known as bispinors), two of which resemble the Pauli wavefunction in the non-relativistic limit, in contrast to the Schrödinger equation which described wave functions of only one complex value. Moreover, in the limit of zero mass, the Dirac equation reduces to the Weyl equation. Although Dirac did not at first fully appreciate the importance of his results, the entailed explanation of spin as a consequence of the union of quantum mechanics and relativity—and the eventual discovery of the positron—represents one of the great triumphs of theoretical physics. -
A Tale of Three Equations: Breit, Eddington-Gaunt, and Two-Body
View metadata, citation and similarA Tale papers of at Three core.ac.uk Equations: Breit, Eddington-Gaunt, and Two-Body Dirac brought to you by CORE Peter Van Alstine provided by CERN Document Server 12474 Sunny Glenn Drive, Moorpark, Ca. 90125 Horace W. Crater The University of Tennessee Space Institute Tullahoma,Tennessee 37388 G.Breit’s original paper of 1929 postulates the Breit equation as a correction to an earlier defective equation due to Eddington and Gaunt, containing a form of interaction suggested by Heisenberg and Pauli. We observe that manifestly covariant electromagnetic Two-Body Dirac equations previously obtained by us in the framework of Relativistic Constraint Mechanics reproduce the spectral results of the Breit equation but through an interaction structure that contains that of Eddington and Gaunt. By repeating for our equation the analysis that Breit used to demonstrate the superiority of his equation to that of Eddington and Gaunt, we show that the historically unfamiliar interaction structures of Two-Body Dirac equations (in Breit-like form) are just what is needed to correct the covariant Eddington Gaunt equation without resorting to Breit’s version of retardation. 1 I. INTRODUCTION Three score and seven years ago, Gregory Breit extended Dirac’s spin-1/2 wave equation to a system of two charged particles [1]. He formed his equation by summing two free-particle Dirac Hamiltonians with an interaction obtained by substituting Dirac α~’s for velocities in the semi-relativistic electrodynamic interaction of Darwin:. α 1 EΨ= α~ ·p~ +β m +α~ ·p~ +β m − [1 − (α~ · α~ + α~ · r~ˆ α ·rˆ)] Ψ. -
Arxiv:Hep-Ph/9412261V1 8 Dec 1994
IPNO/TH 94-85 How to obtain a covariant Breit type equation from relativistic Constraint Theory J. Mourad Laboratoire de Mod`eles de Physique Math´ematique, Universit´ede Tours, Parc de Grandmont, F-37200 Tours, France H. Sazdjian Division de Physique Th´eorique∗, Institut de Physique Nucl´eaire, Universit´eParis XI, F-91406 Orsay Cedex, France arXiv:hep-ph/9412261v1 8 Dec 1994 October 1994 ∗Unit´ede Recherche des Universit´es Paris 11 et Paris 6 associ´ee au CNRS. 1 Abstract It is shown that, by an appropriate modification of the structure of the interaction po- tential, the Breit equation can be incorporated into a set of two compatible manifestly covariant wave equations, derived from the general rules of Constraint Theory. The com- plementary equation to the covariant Breit type equation determines the evolution law in the relative time variable. The interaction potential can be systematically calculated in perturbation theory from Feynman diagrams. The normalization condition of the Breit wave function is determined. The wave equation is reduced, for general classes of poten- tial, to a single Pauli-Schr¨odinger type equation. As an application of the covariant Breit type equation, we exhibit massless pseudoscalar bound state solutions, corresponding to a particular class of confining potentials. PACS numbers : 03.65.Pm, 11.10.St, 12.39.Ki. 2 1 Introduction Historically, The Breit equation [1] represents the first attempt to describe the relativistic dynamics of two interacting fermion systems. It consists in summing the free Dirac hamiltonians of the two fermions and adding mutual and, eventually, external potentials. This equation, when applied to QED, with one-photon exchange diagram considered in the Coulomb gauge, and solved in the linearized approximation, provides the correct spectra to order α4 [1, 2] for various bound state problems. -
Solvable Two-Body Dirac Equation As a Potential Model of Light Mesons?
Symmetry, Integrability and Geometry: Methods and Applications SIGMA 4 (2008), 048, 19 pages Solvable Two-Body Dirac Equation as a Potential Model of Light Mesons? Askold DUVIRYAK Institute for Condensed Matter Physics of National Academy of Sciences of Ukraine, 1 Svientsitskii Str., UA–79011 Lviv, Ukraine E-mail: [email protected] Received October 29, 2007, in final form May 07, 2008; Published online May 30, 2008 Original article is available at http://www.emis.de/journals/SIGMA/2008/048/ Abstract. The two-body Dirac equation with general local potential is reduced to the pair of ordinary second-order differential equations for radial components of a wave function. The class of linear + Coulomb potentials with complicated spin-angular structure is found, for which the equation is exactly solvable. On this ground a relativistic potential model of light mesons is constructed and the mass spectrum is calculated. It is compared with experimental data. Key words: two body Dirac equation; Dirac oscillator; solvable model; Regge trajectories 2000 Mathematics Subject Classification: 81Q05; 34A05 1 Introduction It is well known that light meson spectra are structured into Regge trajectories which are approximately linear and degenerated due to a weak dependence of masses of resonances on their spin state. These features are reproduced well within the exactly solvable simple relativistic oscillator model (SROM) [1, 2, 3] describing two Klein–Gordon particles harmonically bound. Actually, mesons consist of quarks, i.e., spin-1/2 constituents. Thus potential models based on the Dirac equation are expected to be more appropriate for mesons spectroscopy. In recent years the two body Dirac equations (2BDE) in different formulations1 with various confining potentials are used as a relativistic constituent quark models [16, 17, 18, 19, 20, 21, 22, 23, 24, 25, 26]. -
Dirac-Exact Relativistic Methods: the Normalized Elimination of the Small Component Method† Dieter Cremer,∗ Wenli Zou and Michael Filatov
Advanced Review Dirac-exact relativistic methods: the normalized elimination of the small component method† Dieter Cremer,∗ Wenli Zou and Michael Filatov Dirac-exact relativistic methods, i.e., 2- or 1-component methods which exactly reproduce the one-electron energies of the original 4-component Dirac method, have established a standard for reliable relativistic quantum chemical calculations targeting medium- and large-sized molecules. Their development was initiated and facilitated in the late 1990s by Dyall’s development of the normalized elimination of the small component (NESC). Dyall’s work has fostered the conversion of NESC and related (later developed) methods into routinely used, multipurpose Dirac- exact methods by which energies, first-order, and second-order properties can be calculated at computational costs, which are only slightly higher than those of nonrelativistic methods. This review summarizes the development of a generally applicable 1-component NESC algorithm leading to the calculation of reliable energies, geometries, electron density distributions, electric moments, electric field gradients, hyperfine structure constants, contact densities and Mossbauer¨ isomer shifts, nuclear quadrupole coupling constants, vibrational frequencies, infrared intensities, and static electric dipole polarizabilities. In addition, the derivation and computational possibilities of 2-component NESC methods are discussed and their use for the calculation of spin-orbit coupling (SOC) effects in connection with spin-orbit splittings and SOC-corrected -
Eigenvalues of the Breit Equation
Prog. Theor. Exp. Phys. 2013, 063B03 (13 pages) DOI: 10.1093/ptep/ptt041 Eigenvalues of the Breit equation Yoshio Yamaguchi1,† and Hikoya Kasari2,∗ 1Nishina Center, RIKEN, 350-0198 2-1 Hirosawa, Wako, Saitama, Japan 2Department of Physics, School of Science, Tokai University 259-1292 4-1-1 Kitakaname, Hiratsuka, Kanagawa, Japan ∗E-mail: [email protected] Received January 9, 2013; Accepted April 12, 2013; Published June 1, 2013 ............................................................................... Eigenvalues of the Breit equation Downloaded from e2 (α p + β m)αα δββ + δαα (−α p + β M)ββ − δαα δββ αβ = Eαβ , 1 1 2 2 r in which only the static Coulomb potential is considered, have been found. Here a detailed 1 discussion of the simple cases, S0, m = M, and m = M, is given, deriving the exact energy eigenvalues. An α2 expansion is used to find radial wave functions. The leading term is given by http://ptep.oxfordjournals.org/ the classical Coulomb wave function. The technique used here can be applied to other cases. ............................................................................... Subject Index B87 1. Introduction and the Breit equation at CERN LIBRARY on June 21, 2013 1.1. Introduction The Breit equation [1–3] has traditionally [4] been considered to be singular, and no attempt has ever been made to solve it. Instead, the Pauli approximation or a generalized Foldy–Wouthuysen trans- formation has been applied to derive the effective Hamiltonian Heff, consisting of the Schrödinger Hamiltonian 1 1 1 e2 H =− + p2 − 0 2 m M r and many other relativistic correction terms [4–6]. The perturbation method was then used to evaluate the eigenvalues (binding energies) in a power series with α as high as possible (or as high as necessary for experimental verification of quantum electrodynamics). -
On the Spectra of Atoms and Hadrons
TTP/05-22 Nov. 2005 On the spectra of atoms and hadrons Hartmut Pilkuhn Institut f¨ur Theoretische Teilchenphysik, Universit¨at, D-76128 Karlsruhe, Germany For relativistic closed systems, an operator is explained which has as stationary eigenvalues the squares of the total cms energies, while the wave function has only half as many components as the corresponding Dirac wave function. The operator’s time dependence is generalized to a Klein-Gordon equation. It ensures relativistic kinematics in radiative decays. The new operator is not hermitian. Energy levels of bound states are calculated by a variety of methods, which include relativity at least approximately. In atomic theory, the equation HψD = EψD is used, where H is the n-body Dirac-Breit Hamiltonian, and ψD is an n-electron Dirac spinor with 4n components. For half a century, great hopes were attached to the Bethe-Salpeter equation, for example in the calculation of positronium spectra [1]. Most of these methods have been adapted to hadrons, namely to mesons as quark-antiquark bound states and baryons as three-quark bound states. New methods such as nonrelativistic quantum electro- dynamics (NRQED) and numerical calculations on a space-time lattice have been added. In this note, the recent extension of another new method to radiative decays is presented. 2 2 Its time-independent form is similar to HψD = EψD, namely M ψ = E ψ, but ψ has only half as many components as ψD. It applies only to closed systems, where E denotes the total cms energy. For atoms, this implies a relativistic inclusion of the nucleus, which is of little practical importance. -
Chemistry of the Noble Gases*
CHEMISTRY OF THE NOBLE GASES* By Professor K. K. GREE~woon , :.\I.Sc., sc.D .. r".lU.C. University of N ewca.stle 1tpon Tyne The inert gases, or noble gases as they are elements were unsuccessful, and for over now more appropriately called, are a remark 60 years they epitomized chemical inertness. able group of elements. The lightest, helium, Indeed, their electron configuration, s2p6, was recognized in the gases of the sun before became known as 'the stable octet,' and this it was isolated on ea.rth as its name (i]A.tos) fotmed the basis of the fit·st electronic theory implies. The first inert gas was isolated in of valency in 1916. Despite this, many 1895 by Ramsay and Rayleigh; it was named people felt that it should be possible to induce argon (apy6s, inert) and occurs to the extent the inert gases to form compounds, and many of 0·93% in the earth's atmosphere. The of the early experiments directed to this end other gases were all isolated before the turn have recently been reviewed.l of the century and were named neon (v€ov, There were several reasons why chemists new), krypton (KpVn'TOV, hidden), xenon believed that the inert gases might form ~€vov, stmnger) and radon (radioactive chemical compounds under the correct con emanation). Though they occur much less ditions. For example, the ionization poten abundantly than argon they cannot strictly tial of xenon is actually lower than those of be called rare gases; this can be illustrated hydrogen, nitrogen, oxygen, fl uorine and by calculating the volumes occupied a.t s.t.p. -
Arxiv:Atom-Ph/9605005V1 22 May 1996
TTP96–16 atom-ph/9605005 Mai 1996 HYPERFINE INTERACTIONS BETWEEN ELECTRONS Ruth H¨ackl and Hartmut Pilkuhn Institut f¨ur Theoretische Teilchenphysik, Universit¨at Karlsruhe, Postfach 6980, D–76228 Karlsruhe, Germany arXiv:atom-ph/9605005v1 22 May 1996 ——– Internet : [email protected] [email protected] Abstract The relativistic Breit Hamiltonian between electrons is transformed into an effective vector potential Ai for the i.th electron, Ai having the structure of a recoil–corrected hyperfine operator. Apart from a small three–body oper- ator, the Dirac–Breit equation is now easier applied to relativistic magnetic properties of complex systems. Relativistic n–electron systems of atoms or molecules are quite precisely described by the Dirac–Breit equation [1]. In addition to the ordinary Dirac–Coulomb Hamiltonian, the equation contains the Breit Hamiltonian [2] 2 α α HB = X Bij , Bij = −e ( i j + αirαjr)/2rij , (1) i<j where the α are Dirac matrices and αir and αjr are the components of αi and αj along the direction ˆr of ri − rj. HB contributes to the electronic fine structure. The term hyperfine interaction is normally reserved for the interaction with the nuclear spin [3]. Breit operators are somewhat inconvenient. Firstly, HB is the only operator in the Dirac–Breit equation which exchanges large and small components of two electrons simulta- neously. Secondly, the use of HB beyond first–order perturbation theory requires complicated 2 improved versions of Bij [4]. This is so because Bij is too large. In this letter we present a transformation which removes both inconveniences. -
The Noble Gases
INTERCHAPTER K The Noble Gases When an electric discharge is passed through a noble gas, light is emitted as electronically excited noble-gas atoms decay to lower energy levels. The tubes contain helium, neon, argon, krypton, and xenon. University Science Books, ©2011. All rights reserved. www.uscibooks.com Title General Chemistry - 4th ed Author McQuarrie/Gallogy Artist George Kelvin Figure # fig. K2 (965) Date 09/02/09 Check if revision Approved K. THE NOBLE GASES K1 2 0 Nitrogen and He Air P Mg(ClO ) NaOH 4 4 2 noble gases 4.002602 1s2 O removal H O removal CO removal 10 0 2 2 2 Ne Figure K.1 A schematic illustration of the removal of O2(g), H2O(g), and CO2(g) from air. First the oxygen is removed by allowing the air to pass over phosphorus, P (s) + 5 O (g) → P O (s). 20.1797 4 2 4 10 2s22p6 The residual air is passed through anhydrous magnesium perchlorate to remove the water vapor, Mg(ClO ) (s) + 6 H O(g) → Mg(ClO ) ∙6 H O(s), and then through sodium hydroxide to remove 18 0 4 2 2 4 2 2 the carbon dioxide, NaOH(s) + CO2(g) → NaHCO3(s). The gas that remains is primarily nitrogen Ar with about 1% noble gases. 39.948 3s23p6 36 0 The Group 18 elements—helium, K-1. The Noble Gases Were Kr neon, argon, krypton, xenon, and Not Discovered until 1893 83.798 radon—are called the noble gases 2 6 4s 4p and are noteworthy for their rela- In 1893, the English physicist Lord Rayleigh noticed 54 0 tive lack of chemical reactivity. -
00419717.Pdf
APPROVED FOR PUBLIC RELEASE APPROVED FOR PUBLIC RELEASE APPROVED FOR PUBLIC RELEASE ~ ,—- UNWMFIED — PUBUCLYREI-EMABLF . ,$5 ~ .~16f3 This Document Consists of 18 Pages /“ @ LQS ALAMOS SCIENTIFIC LABORATORY Contribution from Chemistry-MetallurgyDivision E. R. Jette, Division Leader J. F, Lemons, Group Leader Plutonium~‘=Hexaf uor e: Preparation and Properties w A. E. Flor November 9, 1950 — ‘1” Chemistry-Tranwrs.nicElements “-+ - ,- —. 1 Y– -t APPROVED FOR PUBLIC RELEASE — APPROVED FOR PUBLIC RELEASE LA-I.M8 UNCLASSIFIED Los tiSDIOS 1-20 STANDARD DISTRIBUTION Argonne,I?ationslLaboratory 21-30 Atomic Energy Commission, Washington 31-32 Brookhaven National Laboratory 33-36 Carbide and Carbon Cheticals Division (K-25 Plant) 37-38 Carbide and Carbon Chemicsl.sDivision (Y-12 Plant) General.Electric Company, Richland Z-45 Hanford Operations Office 46 Iowa State College 47 Kellex Corporation 4.$ Knolls Atomic Power Laboratory g-;; Mound Laboratory Navel Radiological Defense Laboratory 56- NEPA Project 57 New York Operations Office 58-59 Oak Ridge National Laboratory 60-65 Patent Branch, Washington 66 Technical Information Division, ORE 6741 UCLA Medical Research Laboratory (Warren) University of California Radiatio nLaboratory %85 University of Rochester 86-87 2 APPROVED FOR PUBLIC RELEASE — APPROVED FOR PUBLIC RELEASE Introduction It is the purpose of this paper to present the results of experi- mental investigations on the chemistry of plutonium hernfluoride con- ducted at this laboratory subsequent to the preparation of report LAMS 1118(1). A more satisfactory apparatus for the preparation is des- cribed. More reliable values for the vapor pressure have been obtained and the related physical constants have been calculated. The rate of decomposition of the compound as a result of the associated alpha radiation has been determined and a preliminary observation on the thermal stability is reported. -
Equivalence of a New Wave Equation to the Breit and Salpeter Equations* Abstract
SLAC-PUB-5633 August 1991 T EQUIVALENCE OF A NEW WAVE EQUATION TO THE BREIT AND SALPETER EQUATIONS* JOHNH. CONNELL Springfield Technical Community College** Armory Square, Springfield, MA 01105 and Stanford Linear Accelerator Center Stanford University, Stanford, California 94309 ABSTRACT It is proven that a recently derived simple configuration-space wave equation for two spin-l/2 particles is equivalent to the Breit equation and to the Salpeter equation in first order perturbation theory. The wave equation is based on a sim- ple quasipotential approximation. The potential in the equation is given by the Blankenbecler-Sugar correction series. The proof holds for an arbitrary combina- tion of scalar and vector interactions. Submitted to Physical Review D, Brief Reports * Work supported in part by the Department of Energy, Contract No. DE-AC03-76SF00515 and Associated Western Universities-DOE Summer Faculty Fellowship. ** Permanent address. Interest in S-dimensional two-body bound state equations for spin-l/2 particles has revived in the last 15 years, due to the success of the qij model of mesons. But two important questions have not been answered yet [1,2]. (1) What equation is best? (2) What interaction is best? This note is about equations. Two have dominated: the Breit equation [3] and Salpeter’s reduction [4] of the Bethe-Salpeter equation [5]. As we shall explain below, neither of these “big two” equations can be solved numerically exactly in configuration space. They are only solved in first-order perturbation theory, which is trusted most for non-relativistic systems. Here we will prove the equivalence in first order perturbation theory of these two equations to a recently derived third equation [6] which h as f avorable configuration space behaviour and may be susceptible to an exact numerical solution.