Ken G said:
But you are not talking about anything quantifiable or repeatable, what is quantifiable and repeatable is that we have no evidence for any non-flatness in our universe, that's it.
Absence of evidence is not evidence of absence. We have observational constraints on the levels of flatness, which are consistent with zero but do not rule out non-zero models.
That is not true at all. All origins stories are going to involve some step that is essentially magical, what matters is whether or not it gives us testable hypotheses. Now, what testable hypotheses is your creation story giving us? None, zilch.
CMB correlation functions. Nucleosynthetic abundances. GUT particle predictions.
The inflation mechanism is still quite vague, and figuring out the flatness or lack therefore of the universe will pin down the mechanism.
There's also theoretical consistency. It turns out that you *can* do a lot of cosmology assuming that GR is wrong and that the universe is Newtonian. The trouble is that when you do that, you run into huge problems when you start putting in a finite speed of light.
No, it predicts the curvature will never be observable.
This is false. Inflation predicts no such thing. Let's ask Alan Guth what he thinks...
http://arxiv.org/abs/1203.6876
What can the observation of nonzero curvature tell us?
It turns out that curvature is a very good probe of the details of the inflation mechanism.
It certainly does not say it isn't zero, it says we have no idea so there are no testable hypotheses around the issue. That further says that there is no point in including curvature in our models, since it is a complication that offers us no testable advantages.
Alan Guth seems to disagree.
Also see
http://arxiv.org/abs/1104.3629
The Primordial Curvature Perturbation from Vector Fields of General non-Abelian Groups
http://arxiv.org/abs/1104.3494
Observational signatures of a non-singular bouncing cosmology
(There are dozens of other papers)
In any case, you can't remove curvature since you are using a gravity model that is based on the concept of curvature. A lot of the experimental tests in cosmology involve measure density perturbations, and even if you are in a universe that is "flat" at the large scale, you have to take into account local curvature if you want to use GR (i.e. the back reaction problem)
http://arxiv.org/abs/1112.5335
Backreaction in late-time cosmology
http://arxiv.org/abs/1203.2635
Inflationary perturbation theory is geometrical optics in phase space
http://arxiv.org/abs/1203.0125
Effect of cosmic backreaction on the future evolution of an accelerating universe