\(h_o=2\pi a_{ \psi }mc\)
is not a mistake. That, this is the case of many particles of different \(a_\psi\), superimposed onto a common center. And that a particle dropping from a higher \(a_\psi\) to a lower valued \(a_\psi\) does emitted a photon.
At this point we don't have a picture of orbiting particles.
However, from the post "Positively Charged Absurdity", we do have two particles with a common \(a_\psi\) superimposed together producing a outward positive \(F\) (Newtonian) around them.
A particle with \(a_\psi\) has a negative \(F\) between zero and \(a_\psi\), so such a particle is attracted to other particles of the same type within the circle transcribed by \(a_\psi\) but is repulsive to other particles of the same type beyond the same circle.
Two particles on each others' \(a_\psi\) circle is attracted to each other and as a pair repulse other particles of the same type. They present themselves as a peculiar stable pair.
If particles interact at sufficiently great distances that the solutions to \(F_\rho\) and \(\psi\) for the particles involved does not change, then their interactions can be regarded as the particles with a constant force field around them. For example, a charge with a E field around it or a mass with a gravity field around it.
If however, the particles are at close proximity, then their \(F_\rho\) interacts as shown by the graph below,
Within an interaction distance of \(x=5\), the shape of the \(F_\rho\) curve and so, the \(\psi\) curve changes. Beyond \(x=5\), individual particles' \(F_\rho\) curves add like integer.
\(\cfrac { G }{ \sqrt { 2{ mc^{ 2 } } } }x_b=5\)
\(x_b=5\cfrac{\sqrt { 2{ mc^{ 2 } } }}{G}\)
where \(x_b\) is the boundary between wave and particle interaction. In this context, wave interactions are defined as when such interactions result in changes to \(\psi\) around the particle(s).
