Three out of four complex components of the Dirac spinor can be algebraically eliminated from the Dirac equation (if some linear combination of electromagnetic fields does not vanish), yielding a partial differential equation of the fourth order for the remaining complex component. This equation is generally equivalent to the Dirac equation. Furthermore, following Schrödinger [Nature (London), 169, 538 (1952)], the remaining component can be made real by a gauge transform, thus extending to the Dirac field the Schrödinger conclusion that charged fields do not necessarily require complex representation. One of the two resulting real equations for the real function describes current conservation and can be obtained from the Maxwell equations in spinor electrodynamics (the Dirac-Maxwell electrodynamics). As the Dirac equation is one of the most fundamental equations, these results both belong in textbooks and can be used for development of new efficient methods and algorithms of quantum chemistry.

1.
R.
Ahuja
,
A.
Blomqvist
,
P.
Larsson
,
P.
Pyykkö
, and
P.
Zaleski-Ejgierd
,
Phys. Rev. Lett.
106
,
018301
(
2011
).
2.
Fayyazuddin
and
Riazuddin
,
Quantum Mechanics
(
World Scientific
,
Singapore
,
1990
).
3.
V. G.
Bagrov
and
D. M.
Gitman
,
Exact Solutions of Relativistic Wave Equations
(
Kluwer
,
Dordrecht
,
1990
).
4.
E.
Schrödinger
,
Nature (London)
169
,
538
(
1952
).
5.
E.
Deumens
,
Physica
18D
,
371
(
1986
).
6.
C.
Itzykson
and
J.-B.
Zuber
,
Quantum Field Theory
(
McGraw-Hill
,
New York
,
1980
).
7.
A.
Akhmeteli
,
Int. J. Quantum Inf.
9
,
17
(
2011
).
8.
V. G.
Bagrov
, private communication (
2010
).
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