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The Angular Momentum Operator in the Dirac Equation
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CENTRE DE PHYSIQUE THEORIQUE - CNRS - Luminy, Case 907
F-13288 Marseille Cedex 9 - France
Unite? Propre de Recherche 7061
The angular momentum operator in the Dirac equation
V??ctor M. Villalba1
Abstract
The Dirac equation in spherically symmetric fields is separated in two different tetrad
frames. One is the standard cartesian (fixed) frame and the second one is the diagonal
(rotating) frame. After separating variables in the Dirac equation in spherical coordinates,
and solving the corresponding eingenvalues equations associated with the angular operators,
we obtain that the spinor solution in the rotating frame can be expressed in terms of Jacobi
polynomials, and it is related to the standard spherical harmonics, which are the basis
solution of the angular momentum in the Cartesian tetrad, by a similarity transformation
Key-Words : 3.65, 11.10, 4.90.
April 1994
CPT-94/P.3027
anonymous ftp or gopher: cpt.univ-mrs.fr
1permanent address: Centro de F??sica, Instituto Venezolano de Investigaciones Cient??ficas IVIC, Apdo.
21827, Caracas 1020-A Venezuela
e-mail address: villalba@cpt.univ-mrs.fr, villalba@dino.conicit.ve
1 Introduction
The Dirac equation is a system of four coupled partial differential equation which describes
the relativistic electron and other spin 1/2 particles. Despite the remarkable effort made
during the last decades in order to find exact solutions for the relativistic electron in the
presence of external fields, the amount of solvable problems is relatively scarce, being the
Coulomb problem [1], the plane wave [2], and some electromagnetic configurations [3] the
most representative examples. The problem of finding exact solutions of the Dirac equation
is closely related to the possibility of accomplishing a complete separation of variables of
the Dirac equation.
During the last decades there have been different approaches to tackling the problem
of separating variables in the Dirac
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