Charge Conjugation Symmetry in the Finite Basis Approximation of the Dirac Equation
Four-component relativistic atomic and molecular calculations are typically performed within the no-pair approximation where negative-energy solutions are discarded. These states are, however, needed in QED calculations, wherein, furthermore, charge conjugation symmetry, which connects electronic an...
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doaj-3e71bbfdb76d4507a3dacdf943fce4a02020-11-25T03:49:53ZengMDPI AGSymmetry2073-89942020-07-01121121112110.3390/sym12071121Charge Conjugation Symmetry in the Finite Basis Approximation of the Dirac EquationMaen Salman0Trond Saue1Laboratoire de Chimie et Physique Quantique, UMR 5626 CNRS, Université Toulouse III-Paul Sabatier, 118 Route de Narbonne, F-31062 Toulouse, FranceLaboratoire de Chimie et Physique Quantique, UMR 5626 CNRS, Université Toulouse III-Paul Sabatier, 118 Route de Narbonne, F-31062 Toulouse, FranceFour-component relativistic atomic and molecular calculations are typically performed within the no-pair approximation where negative-energy solutions are discarded. These states are, however, needed in QED calculations, wherein, furthermore, charge conjugation symmetry, which connects electronic and positronic solutions, becomes an issue. In this work, we shall discuss the realization of charge conjugation symmetry of the Dirac equation in a central field within the finite basis approximation. Three schemes for basis set construction are considered: restricted, inverse, and dual kinetic balance. We find that charge conjugation symmetry can be realized within the restricted and inverse kinetic balance prescriptions, but only with a special form of basis functions that does not obey the right boundary conditions of the radial wavefunctions. The dual kinetic balance prescription is, on the other hand, compatible with charge conjugation symmetry without restricting the form of the radial basis functions. However, since charge conjugation relates solutions of opposite value of the quantum number <inline-formula> <math display="inline"> <semantics> <mi>κ</mi> </semantics> </math> </inline-formula>, this requires the use of basis sets chosen according to total angular momentum <i>j</i> rather than orbital angular momentum <i>ℓ</i>. As a special case, we consider the free-particle Dirac equation, where opposite energy solutions are related by charge conjugation symmetry. We show that there is additional symmetry in that solutions of the <i>same</i> value of <inline-formula> <math display="inline"> <semantics> <mi>κ</mi> </semantics> </math> </inline-formula> come in pairs of opposite energy.https://www.mdpi.com/2073-8994/12/7/1121Dirac equationfinite basis approximationcharge conjugation symmetrykinetic balance |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Maen Salman Trond Saue |
spellingShingle |
Maen Salman Trond Saue Charge Conjugation Symmetry in the Finite Basis Approximation of the Dirac Equation Symmetry Dirac equation finite basis approximation charge conjugation symmetry kinetic balance |
author_facet |
Maen Salman Trond Saue |
author_sort |
Maen Salman |
title |
Charge Conjugation Symmetry in the Finite Basis Approximation of the Dirac Equation |
title_short |
Charge Conjugation Symmetry in the Finite Basis Approximation of the Dirac Equation |
title_full |
Charge Conjugation Symmetry in the Finite Basis Approximation of the Dirac Equation |
title_fullStr |
Charge Conjugation Symmetry in the Finite Basis Approximation of the Dirac Equation |
title_full_unstemmed |
Charge Conjugation Symmetry in the Finite Basis Approximation of the Dirac Equation |
title_sort |
charge conjugation symmetry in the finite basis approximation of the dirac equation |
publisher |
MDPI AG |
series |
Symmetry |
issn |
2073-8994 |
publishDate |
2020-07-01 |
description |
Four-component relativistic atomic and molecular calculations are typically performed within the no-pair approximation where negative-energy solutions are discarded. These states are, however, needed in QED calculations, wherein, furthermore, charge conjugation symmetry, which connects electronic and positronic solutions, becomes an issue. In this work, we shall discuss the realization of charge conjugation symmetry of the Dirac equation in a central field within the finite basis approximation. Three schemes for basis set construction are considered: restricted, inverse, and dual kinetic balance. We find that charge conjugation symmetry can be realized within the restricted and inverse kinetic balance prescriptions, but only with a special form of basis functions that does not obey the right boundary conditions of the radial wavefunctions. The dual kinetic balance prescription is, on the other hand, compatible with charge conjugation symmetry without restricting the form of the radial basis functions. However, since charge conjugation relates solutions of opposite value of the quantum number <inline-formula> <math display="inline"> <semantics> <mi>κ</mi> </semantics> </math> </inline-formula>, this requires the use of basis sets chosen according to total angular momentum <i>j</i> rather than orbital angular momentum <i>ℓ</i>. As a special case, we consider the free-particle Dirac equation, where opposite energy solutions are related by charge conjugation symmetry. We show that there is additional symmetry in that solutions of the <i>same</i> value of <inline-formula> <math display="inline"> <semantics> <mi>κ</mi> </semantics> </math> </inline-formula> come in pairs of opposite energy. |
topic |
Dirac equation finite basis approximation charge conjugation symmetry kinetic balance |
url |
https://www.mdpi.com/2073-8994/12/7/1121 |
work_keys_str_mv |
AT maensalman chargeconjugationsymmetryinthefinitebasisapproximationofthediracequation AT trondsaue chargeconjugationsymmetryinthefinitebasisapproximationofthediracequation |
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