2 2 8 D O C . 5 4 A D D I T I O N T O G E N E R A L R E L A T I V I T Y
Compared to the original form of the general theory of relativity, the whole novelty
consists then only in the addition of the differential equation (6), which the
must obey.
Our only intention was to point out a logical possibility that is worthy of publi-
cation; it may be useful for physics or not. Only further investigations can show
whether one or the other is the case, and if there is more to be considered than one
Weyl invariant .
Translator’s Note
{1} The misprint has been corrected to .
T g) ( 0. =
gμν
[9]
J H =
[10][11]{1}
K H
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