If \(a_\psi\) can be as large as a planet, then it is possible to create a \(\psi\), \(x_z=0\), where the force field is positive outwards. Such a field would act as a shield, decelerating objects that come onwards.
\(a_\psi=n\cfrac{\lambda}{2\pi }\)
If electron corresponds to \(a_\psi=14.77\) nm
\(_na_\psi=n14.77\) nm
when \(n=5\times10^7\)
\(_na_\psi=0.7385\) m
where even numbers of electron circulates in a circular confinement. In case, \(F_\rho\) does not add up,
where each radius, \(r_n\) satisfies,
\(r_n=\,_na_\psi=n14.77\) nm
The electron pairs should resonate naturally. Their \(\psi\) profile is that of a single big particle with \(F_\rho\) positive outwards.