Abstract
AbstractThe gyroscopic invariance implies the representation of the antisymmetric part of the Hermite‐symmetric metric by a vector potential. Therefore we introduce the six functions of this antisymmetric part in general as derived by two vector potentials. Then Einstein's variational principle leads to a slight modification of the Einstein‐Schrödinger equations, which just encludes Minkowski's form of the energy‐momentum tensor for the electromagnetic field and the gluon field.
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