) of the volume element
will equal zero and no preference can be given to any direction. Then it can be shown that the form of the function is given by
where
,
are integration constants which stand in a certain relation to each other, namely,
) of the volume element
will equal zero and no preference can be given to any direction. Then it can be shown that the form of the function is given by
where
,
are integration constants which stand in a certain relation to each other, namely,