As for your own approach, the laws of Relativity aren't set in stone, but you're only offering "maybe's" as an alternative. When your theory can explain results such as the Bell experiments and other established quantum phenomena, and can answer all the questions as to what we're supposed to replace Relativity with, only then can you claim to have a working theory. Right now it sounds like you only have an outline of what you'll hope to achieve based on modifying previously unsuccessful approaches, but hopes don't amount to a math proof.
Sorry, but my theory of gravity is not a maybe, but a published well-defined theory, and it has quite definite properties. First of all, it has a preferred frame.
With this preferred frame, standard de Broglie-Bohm theory can be used in the context of relativistic gravity too. But standard de Broglie-Bohm theory is sufficient to solve all the "measurement problems" and to explain, but its not very hidden "hidden variable", the outcome of Bell experiments.
To my understanding, all it does is sweep the randomness seen in experiments under the rug by attributing it to hidden players we can't directly observe.
This is, of course, the point of hidden variables. We want to have a reasonable, meaningful explanation how this can happen.
According to this same understanding, deterministic mechanisms have never been specified in such a way as to produce the required statistical outcomes. In pilot wave theory, I haven't seen or heard of any specification whatsoever as to how the pilot wave decides in advance what it's ultimately going to collapse to or how it's going to guide the accompanying particle.
So you simply have to learn elementary dBB theory. It has an equation, the guiding equation, which defines exactly how the wave function guides the configuration:
$$\dot{q}(t) = \nabla \Im \ln \psi(q(t),t)$$. So, we have a complete evolution equation for the wave function (which follows the Schroedinger equation) and the configuration (which follows this guiding equation).
And for the collapse there is also a well-defined formula, which defines the effective wave function of a subsystem:
$$\psi_{eff}(q_{sys},t) = \psi(q_{sys}, q_{env}(t),t)$$
If there is no interaction between the system and the environment, this gives the Schroedinger equation for the effective wavefunction of the subsystem. If there is an interaction, this describes the process of collapse during the measurement process.