exponent137 said:
let us assume, that the universe is without matter all the time. I think that Schwarzschild solution does not exist in such universe
You are incorrect. The Schwarzschild solution is a vacuum solution, so it is a possible solution for a "universe without matter all the time". Any vacuum solution is.
If you were to say that the Schwarzschild solution is not a
physically realistic solution for a universe without matter all the time, I would agree with that; the "white hole" singularity in the full Schwarzschild solution is not, IMO, physically realistic. But to say the solution "does not exist" is not correct; it exists, it just isn't (IMO) physically realistic. Lots of solutions to the EFE exist that aren't physically realistic.
exponent137 said:
I think that such universe has many forms of gravitational waves.
There are also vacuum solutions to the EFE that contain gravitational waves, yes. But they are not the only vacuum solutions. So you can't just assert that a universe without matter
must be one of the gravitational wave solutions. That isn't correct.
I would not even say the vacuum everywhere gravitational wave solutions are more physically realistic than the Schwarzschild solution, because if the universe is vacuum everywhere, there are no sources to produce gravitational waves, so a physically realistic solution should not contain them.
exponent137 said:
It is a consequence of the number of free parameters is larger than it is given by ##G_{\mu\nu}=0##.
I'm not sure what you mean here. If you just mean that the condition ##G_{\mu \nu} = 0## does not pick out a unique solution, of course it doesn't.
exponent137 said:
This is what I thought as initial conditions. Maybe, edge conditions is a better word?
Not really. What differentiates the various types of possible vacuum solutions is something more like symmetry assumptions--for example, spherical symmetry is the key assumption that leads to the Schwarzschild solution. Such assumptions are not really initial conditions or boundary conditions.