Can spacetime be defined by the requirement that the physical laws are simple?

Question

When I was student I was told that time is defined by the requirement that the physical laws are simple. For example, in classical mechanics time can be defined by the requirment that the velocity of an isolated body is constant. One could generalize this approach by assuming that space-time is defined by the requirement that the physical laws are simple. This can be easily expressed in mathematical language as follows.

In general relativity the universe is represented by the triple $(M, g, T)$ where $M$ is a four-dimensional differentiable manifold, $g$ is a Lorentzian metric, and $T$ is a matter tensor field on $M$ satisfying Einstein's equation.

According to the above approach, we could say that the "true" physical reality of the universe is represented by the pair $(M, T)$, while the metric $g$ emerges as an appeareance from the requirement that evolution appears simple, i.e., that $g$ and $T$ satisfy Einstein's equation.

From the mathematical point of view, this approach poses for example the following problems: does any matter tensor field $T$ admit a metric $g$ such that Einstein's equation is satisfied? To what extent a tensor field $T$ univocally determines the metric $g$?

Does this approach make sense, at least from the mathematical point of view?

Answer 1

Addressing just the last two paragraphs of your question:

If $T$ is "non-degenerate" (at every point as a linear transformation from $T_pM \to T_p^*M$), then modulo some issues with the constraint equations $g$ can be solved from $T$, at least locally in time, after prescribing it in a compatible way on a space-like hypersurface. See this article by De Turck.

Presumeably the issue with degeneracy has more to do with the method involved in solving the problem, then with it being a critical condition, since the evolution for Ricci-flat metrics (Einstein vacuum equations) is also well-posed.

The main difficulty is about the "univocal" part: due to diffeomorphism invariance, the "local" problem for prescribing Ricci curvature is under-determined. (The global problem may have topological constraints; that I am not sure about.) So one expects that for the local problem the issue is more likely the overabundance of solutions.

On the other hand, the prescription of initial/boundary data may be crucial. Roughly speaking the prescribing Ricci curvature equation is analogous to the inhomogeneous wave equation with a source term. In which case the hyperbolic nature of the equations shows that for any initial configuration there exists a different evolution. So it may be that this will lead to multiple different metrics compatible with your $T$ (indeed consider the case where you restrict your manifold to be $M = \mathbb{R}^4$; the global nonlinear stability of Minkowski space, combined with classical results on classical results on the existence of solutions to the vacuum constraint equations shows that on $M = \mathbb{R}^4$ there are many incongruent (since for these other solutions the Weyl tensor is non-vanishing) solutions to Einstein's equation when $T = 0$; I would expect something similar for the case of prescribed $T$).