’s at a point and at the neighbouring points in any mesh-system, so now the distance-curvature at a point can be given by a tensor built up from the changes in values between the
’s at a point and at the neighbouring points in any gauge-system.
In particular, the Weylian curvature
, at a point, is given by the tensor equation
whence we may derive
If the space manifests no trace of distance-curvature, hence no Weylian characteristics,