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Reference9 articles.
1. J. A. Ferrari:Foundations for a theory of gravitation, inNuovo Cimento B,78, 53 (1983).
2. No particular (exclusive) property of static gravitational fields is used to derive this conclusion.
3. In the general case, the transformation equation for lengths could be obtained by using the principle of superposition.
4. SeeN. Rosen:Phys. Rev.,57, 150 (1940). In his words, «… We cannot carry out a Lorentz transformation in the presence of a gravitational field, but must first get rid of the latter by going over to a suitable system in which the componentsg μν [of the metric tensor] are constant (at least for a small portion of space), we can always make a further co-ordinate transformation so as to give them their special relativity values. But then no light-drag or “ether-drift” can be observed».
5. The Fizeau experiment was originally proposed byN. Rosen as an attempt (not rather satisfactory) to explain the well-known results ofD. C. Miller (Rev. Mod. Phys.,5, 203 (1933)) on the «ether drift», and not as a decisive experiment for a scalar theory of gravitation.
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