Abstract
TYABJI1 recently determined the canonical and symmetrical energy momentum tensors of Dirac's2 new theory of electrodynamics. Tyabji used the conventional definition of the canonical energy momentum tensor and symmetrized this tensor in the traditional manner3–5. The canonical tensor
given by Tyabji can be written without the explicit appearance of the ξ and η variables, as follows :
or
The symmetrizing tensor1,
, is
or
(5) simply removes the unsymmetrical mixed term of (2) and adds the ‘matter’ contribution to the energy momentum tensor to yield1
If (3) is added to (4), the canonical tensor contains the ‘matter’ term, and the symmetrizing tensor cancels the mixed last term of (3). λ is a scalar function of xµ, and can be interpreted as the rest mass density of the streams of electrical charge.
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References
Tyabji, S. F. B., Nature, 170, 116 (1952).
Dirac, P. A. M., Proc. Roy. Soc., A, 212, 330 (1952).
Belinfante, F. J., Physica, 6, 887 (1939).
Iskraut, R. W., Z. Phys., 119, 659 (1942).
Wentzel, G., “Quantum Theory of Fields” (1949).
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ISKRAUT, R. Angular Momentum in Dirac's New Electrodynamics. Nature 170, 1125–1126 (1952). https://doi.org/10.1038/1701125a0
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DOI: https://doi.org/10.1038/1701125a0


