Friedrich Kottler, Translation:On the spacetime lines of a Minkowski world…
“ If we treat as covariant, then this is evidently somewhat arbitrary in terms of Cartesian orthogonal coordinates, since covariants and contravariantes coincide here. If we would require (following Abraham) that the transform like the products of the corresponding components of the radius vector, then we would have to postulate the as contravariants. By passage to the reciprocal system we can, however, represent them as convariants. For the sake of being easier related to the integral forms, we stick to the covariant description. ”
