Dirac-Exact Relativistic Methods: the Normalized Elimination of the Small Component Method† Dieter Cremer,∗ Wenli Zou and Michael Filatov
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Rainbow 18C PT 0318 Ad Ge訂正
1 18 1 H 2 He 1.008 4.003 hydrogen Rainbow Periodic Table helium 2.20 +1 guide☆ 1 with Quad electron data atomic number 82 Pb symbol 1 atomic weight 207.2 categories(Wikipedia): 2 -1 2 name 13 14 15 16 17 lead known oxidation state Alkali metals Post-transition metals 3 Li 4 Be electronegativity 2.33 +4 highest Alkaline earth metals Metalloids 5 B 6 C 7 N 8 O 9 F 10 Ne 14 [ ]:common Transition metals Reactive nonmetals 6.941 9.012 Quad electron data 10.81 12.01 14.01 16.00 19.00 20.18 lithium beryllium 2 10 [ ]:uncommon Lanthanides Noble gases boron carbon nitrogen oxygen fluorine neon 14 10 2 2 2 2 0.98 +1 1.57 +2 [Xe] 4f 5d 6s 6p [Xe] -4 lowest Actinides Unknown chemical properties 2.04 +3 2.55 +4 3.04 +5 3.44 +2 3.98 -1 shells 1 2 3 4 5 6 1 2 l=3 2 2 2 2 2 2 [He] +1 [He] +1 n=1 n=2 n=3 n=4 n=5 n=6 n=7 n=8 [He] -5 [He] -4 [He] -3 [He] -2 [He] -1 [He] f 11 Na 12 Mg orbitals l=1 p d l=2 13 Al 14 Si 15 P 16 S 17 Cl 18 Ar 22.99 24.31 s 26.98 28.09 30.97 32.07 35.45 39.95 sodium magnesium K L M N O P Q R aluminium silicon phosphorus sulfur chlorine argon 0.93 +1 1.31 +2 l=0 nickname*: 'Ketchup' 'MustardYellow' 'Ocean Blue' 'Quin Violet' 1.61 +3 1.90 +4 2.19 +5 2.58 +6 3.16 +7 3 'Ladyfinger' 'NatureGreen' 'Pansy Blue' 'Ricecake' * suggested by Valery Tsimmerman 1 2 3 4 5 6 1 2 2 2 2 2 2 2 [Ne] -1 [Ne] +1 3 4 5 6 7 8 9 10 11 12 [Ne] -2 [Ne] -4 [Ne] -3 [Ne] -2 [Ne] -1 [Ne] 19 K 20 Ca 21 Sc 22 Ti 23 V 24 Cr 25 Mn 26 Fe 27 Co 28 Ni 29 Cu 30 Zn 31 Ga 32 Ge 33 As 34 Se 35 Br 36 Kr 39.10 40.08 44.96 47.87 50.94 52.00 54.94 55.85 58.93 58.69 63.55 -
Classification of Elements and Periodicity in Properties
74 CHEMISTRY UNIT 3 CLASSIFICATION OF ELEMENTS AND PERIODICITY IN PROPERTIES The Periodic Table is arguably the most important concept in chemistry, both in principle and in practice. It is the everyday support for students, it suggests new avenues of research to After studying this Unit, you will be professionals, and it provides a succinct organization of the able to whole of chemistry. It is a remarkable demonstration of the fact that the chemical elements are not a random cluster of • appreciate how the concept of entities but instead display trends and lie together in families. grouping elements in accordance to An awareness of the Periodic Table is essential to anyone who their properties led to the wishes to disentangle the world and see how it is built up development of Periodic Table. from the fundamental building blocks of the chemistry, the understand the Periodic Law; • chemical elements. • understand the significance of atomic number and electronic Glenn T. Seaborg configuration as the basis for periodic classification; • name the elements with In this Unit, we will study the historical development of the Z >100 according to IUPAC Periodic Table as it stands today and the Modern Periodic nomenclature; Law. We will also learn how the periodic classification • classify elements into s, p, d, f follows as a logical consequence of the electronic blocks and learn their main configuration of atoms. Finally, we shall examine some of characteristics; the periodic trends in the physical and chemical properties • recognise the periodic trends in of the elements. physical and chemical properties of elements; 3.1 WHY DO WE NEED TO CLASSIFY ELEMENTS ? compare the reactivity of elements • We know by now that the elements are the basic units of all and correlate it with their occurrence in nature; types of matter. -
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]. -
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. -
Scientific Literacy Theme : Periodic Classification of Elements Unit 1
SCIENTIFIC LITERACY THEME : PERIODIC CLASSIFICATION OF ELEMENTS UNIT 1 : IUPAC NOMENCLATURE OF ELEMENTS While studying the arrangement of elements Aditya found that there are some elements with atomic number greater than 100 have not named till now as per the periodic table. He tried to find the system to know their names and he found that IUPAC recommended a system of naming new elements till they have given a proper name. the table for naming the elements is given below. With every name a suffix ‘ium’ is added. Digit 0 1 2 3 4 5 6 7 8 9 Root nil un bi tri quad pent hep sept oct Enn abbreviation n u b t q p h s o e Question 1 The IUPAC name for the element with atomic number 120 is (a) Ununquadrdium (b) Unununium (c) Unbinilium (d) unmilennium Question 2 The symbol for IUPAC element unnilquadium is (a) unt (b) unq (c) uno (d) uub Question 3 what is the name and symbol of element with atomic number 118? ------------------------------------------------------------------------------------------------------------------------------- ------------------------------------------------------------------------------------------------------------------------------- Question 4 Write the name and atomic number of element with symbol uuu ------------------------------------------------------------------------------------------------------------------------------- ------------------------------------------------------------------------------------------------------------------------------- UNIT 2 : ELEMENT POSITION IN PERIODIC TABLE Three elements X, -
Periodic Table of the Elements
PERIODIC TABLE OF THE ELEMENTS GROUP 1 18 IA VIIIA 1 1,00794 2 4,002602 Legend Categories Common Constants H He 1 Hydrogen 2,1 Atomic Number 1 1,00794 †Atomic Weight Non Metals Poor Metals Absolute Zero -273.15 °C Fine-structure constant α 0.0072973525 Helium - -27 -11 3 -1 -2 Atomic Mass Unit mu 1.660539x10 kg Gravitation Constant G 6,67408x10 m kg s 23 -1 -1 -1 Symbol Avogadro Constant N 6,022137x10 mol Molar Gas Constant R 8,31451J mol K 2 1s1 2 probable Poor A 13 14 15 16 17 1s H Alkali Metals 3 1,-1 Metals Base of Natural Logarithms e 2.718281828 Molar Volume (Ideal Gas) 0.02241410 m /mol 0 IIA Name Hydrogen 2,2 *Electronegativity Boltzmann constant k 1,380658x10-23 J/K π π 3.14159265358979 IIIA IVA VA VIA VIIA (Pauling) probable Alkali Electron Mass m 9,1093897x10-31 kg Planck Constant h 6,626076x10-34 Js 3 6,941 4 9,012182 e 5 10,811 6 12,011 7 14,00674 8 15,9994 9 18,9984032 10 20,1797 1 Metalloids 2 1s †Electron Configuration Metals 0.510998 MeV/c Proton-Electron Mass Ratio me/mp 1836,15267389 [NOTE] Electron Radius (Classical) r0- 2.8179403x10-15 m Rydberg Constant R 10 973 732 m-1 +1,-1 Possible Oxid. States Alkaline Hearth ∞ Li Be probable Metalloids Electron Volt eV 1.602176x10-19 J Speed of Light in a Vacuum c 299 792 458 m/s B C N O F Ne Metals -19 Lithium 0,98 Beryllium 1,57 Elementry Charge e 1,6021773x10 C Speed of sound in air at STP 343.8 m/s Boron 2,04 Carbon 2,55 Nitrogen 3,04 Oxygen 3,44 Fluorine 3,98 Neon - 2 probable Alkaline Faraday Constant F 9,648531x104 C/mol-1 Standard Pressure 101 325 Pa Phase at STP Halogens -
Spin-Orbit Coupling Calculations with the Two-Component Normalized Elimination of the Small Component Method Michael Filatov, Wenli Zou, and Dieter Cremer
Spin-orbit coupling calculations with the two-component normalized elimination of the small component method Michael Filatov, Wenli Zou, and Dieter Cremer Citation: J. Chem. Phys. 139, 014106 (2013); doi: 10.1063/1.4811776 View online: http://dx.doi.org/10.1063/1.4811776 View Table of Contents: http://jcp.aip.org/resource/1/JCPSA6/v139/i1 Published by the AIP Publishing LLC. Additional information on J. Chem. Phys. Journal Homepage: http://jcp.aip.org/ Journal Information: http://jcp.aip.org/about/about_the_journal Top downloads: http://jcp.aip.org/features/most_downloaded Information for Authors: http://jcp.aip.org/authors THE JOURNAL OF CHEMICAL PHYSICS 139, 014106 (2013) Spin-orbit coupling calculations with the two-component normalized elimination of the small component method Michael Filatov, Wenli Zou, and Dieter Cremer Department of Chemistry, Southern Methodist University, 3215 Daniel Ave., Dallas, Texas 75275-0314, USA (Received 10 March 2013; accepted 9 June 2013; published online 2 July 2013) A new algorithm for the two-component Normalized Elimination of the Small Component (2cNESC) method is presented and tested in the calculation of spin-orbit (SO) splittings for a series of heavy atoms and their molecules. The 2cNESC is a Dirac-exact method that employs the exact two- component one-electron Hamiltonian and thus leads to exact Dirac SO splittings for one-electron atoms. For many-electron atoms and molecules, the effect of the two-electron SO interaction is mod- eled by a screened nucleus potential using effective nuclear charges as proposed by Boettger [Phys. Rev. B 62, 7809 (2000)]. The use of the screened nucleus potential for the two-electron SO inter- action leads to accurate spinor energy splittings, for which the deviations from the accurate Dirac Fock-Coulomb values are on the average far below the deviations observed for other effective one- electron SO operators. -
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.