haushofer said:
Yes, but as this article by Brans shows: the natural approach for people who know SR is ofcourse to describe gravity by a Lorentz scalar, and it is this approach which violates the equivalence principle.
Yes, there were problems regarding the most straight forward descriptions with a scalar (ie, just swapping the derivatives in Newton's theory with the d'Alembertian operator).
But no, that doesn't mean scalar theories generically violate the equivalence principle.
As I already mentioned, there was a theory proposed by Nordstrom before GR that was a scalar theory and did not violate the equivalence principle. Einstein considered it the only real contender to the theory he was working on at the time.
You can read more about it in the introduction in one of the papers atyy linked
http://arxiv.org/abs/gr-qc/0405030
or wiki has an article about Nordstrom's theory as well
http://en.wikipedia.org/wiki/Nordström's_theory_of_gravitation
Bibipandi said:
Thanks for your suggestion. As I understand, the principle of equivalence states that: in small enough regions of spacetime, the laws of physics reduce to those of special relativity; it is impossible to detect the existence of a gravitational field by means of local experiments. The scalar field describes only the gravitational potential (as stated in Newton's theory of gravitation), not the electromagnetic field (described by tensor field), so the scalar field doesn't satisfy the equivalence principle which requires all kinds of experiment (involving electromagnetic experiments). Am I right?
Not quite.
One of the most famous "gravity + EM" tests is the Pound-Rebka "gravitational redshift of light" test. Nordstrom's theory correctly predicted that. Furthermore, his theory did not violate the equivalence principle as you state it there.
However you are correct in that his theory predicted that light does not "bend", while Einstein predicted that it does. I cannot speak to whether or not
all scalar theories will have this result, but probably so considering the EM contribution to the stress-energy tensor is traceless.
The point however, is that the equivalence principle was very useful in guiding the development of gravitational theories (and the first attempts at a scalar relativistic gravitational theory
did run into problems with the equivalence principle), but you cannot rule out scalar theories based just on the equivalence principle.