If for no other reason than because you proposed your favorite interpretation not as an unproveable picture competing (not very successfully) for the attention of the scientific community today, but as The Way Things Really Are. Your description gave no hint that an additional set of fields are needed, which is not the usual formulation of QM.
It's classical particles following classical trajectories determined by a new kind of classical field.
Well, I'd only read your web page at the time.
You have that backwards. QED was derived from Maxwell's equations. Sure, nowadays they impose U(1) symmetry on the Lagrangian and show that QED falls out. But that's a more recent development. QED was derived by taking Maxwell as the foundation and quantizing the fields. There's various ways to do that, but it's usually done through the Lagrangian.
The Maxwell Lagrangian is
L = -1/4 F_ab F^ab - J^a A_a
in both the classical and quantum theories. The action is minimized in both the classical and quantum theories, leading to Euler-Lagrange equations that are the same in both the classical and quantum theories. The stress tensor is defined the same way, the momentum and angular momentum are derived from the stress tensor in the same way for the classical and quantum theories.
Here's a link to a QFT problem set. The only reason it's quantum instead of classical is because this stuff usually isn't covered in classical courses on E&M.
Maxwell's equations exist in a mechanical context-- the transformation rules and the description of state are imposed externally. In the 19th century they were used in a Galilean paradigm. When we went Einsteinian that didn't change Maxwell's equations any more than relativity changes F=dp/dt. When we go quantum we say A_a no longer represent the field, they represent operators that act on the kets. But the equations of motion still look like Maxwell's equations.
There aren't just "some" similarities, and it's no coincidence that those similarities exist. Nearly the entire theoretical machinery of quantum field theory is lifted straight from classical field theory. The fields become operators, the Poisson brackets are multiplied by i*hbar and called commutators, and off we go.
You'd never know that after taking a course in quantum field theory. Very little of that was probably covered in the classical course, and it's introduced in the quantum course on an as-needed basis. So the students are delving deeper into field theory than they had before, possibly working in the second quantized formulation in a significant way for the first time in their lives, introduced to Green's function methods in the guise of photon propagators for the first time except maybe for a short section on scattering in their introductory QM class, solving particle-particle interactions in the quantum context that are more complicated than they had worked with in their classical class... And you wind up with students that can follow some recipies and think they learned stuff that only applies to QM.