In a later year’s summation, Einstein said: “The general theory of relativity is as yet incomplete insofar as it has been able to apply the general principle of relativity satisfactorily only to gravitational fields, but not to the total field. We do not yet know with certainty, by what mathematical mechanism the total field in space is to be described and what the general invariant laws are to which this total field is subject. One thing, however, seems certain: namely, that the general principle of relativity will prove a necessary and effective tool for the solution of the problem of the total field.”
Clearly, in the 2nd sentence, Einstein still believed that this total field is embedded in a background of space not spacetime. This means his zero elements of the symmetric metric tensor properly represent its field values at every point of the quantum vacuum (region devoid of matter and electromagnetic energy). His revised nonsymmetric field allows nonzero values on both sides of the diagonal of the nonsymmetric metric tensor. However, only if all elements are nonzero does the background vanishes. Therefore, a symmetric no background tensor is a Hadamard matrix. Its elements are nonzero and can represent a no background spacetime of squares of quantized energy.


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