In the post "Charge Photons Creation", it was suggested that charges on relaxation from an excited state emit photons of the nature, ph(\(t_c\),\(t_g\)) and ph(\(t_c\),\(t_T\)) where \(t_c\) is the time axis on with the photons exist and \(t_g\), or \(t_T\) is the time axis on which they oscillates.
If the process is reversible, then a photon of the correct nature will impart energy onto charges of the corresponding nature ch(\(t_g\)) or ch(\(t_T\)).
In the post "Amplitude, \(A_n\)", it was suggested that \(\psi\) at \(a_{\psi\,n}\), makes a state transition to the next level, \(a_{\psi\,n+1}\) when its amplitude has gain enough magnitude.
It might be possible to bathe a particle in photons of the correct nature such that its \(a_{\psi\,n}\) increases slowly, and then induce a sudden collapse such that we have,
\(\cfrac{\partial\,E_{\Delta h}}{\partial\,t}\lt0\)
and very large.
As long as the photons shines on the particle,
\(\cfrac{\partial\,E_p}{\partial\,t}=\cfrac{\partial\,E_{\Delta h}}{\partial\,t}\gt0\)
where \(E_p\) is the photon energy,
this itself maybe enough to stop the relaxation of energy states, as \(a_{\psi\,n}\) is prompted to the next higher level continuously. Conversely if the photons are suddenly switched off, the absence of a driving force that increases \(a_{\psi\,n}\) continuously maybe enough to trigger a collapse of energy states, as the particle is now at a very high \(a_{\psi\,n}\). Otherwise, an increase in \(\psi\) from a magnetic/electric field around the particle as the photons are switched off, might prompt a continuous energy state relaxation. Such continuous relaxations are accompanied by emissions of photons at light speed, and are expected to produce a large negative \(\cfrac{\partial\,E_{\Delta h}}{\partial\,t}\).
Teleportation/Warp speed could be as simple as turning a switch on and off. The presence of an external field that would effect \(E_{\Delta h}\) of the particle is important because its rate of change with time must follow the profile,
\(\cfrac{\partial\,E_{\Delta h}}{\partial\,t}=\cfrac{A}{t}\) \(A\lt0\)
over the cascade of transitions to lower \(a_{\psi\,n}\).
How then to generate massive amount of photons of high energy, of a particular nature?
Imagine such a massive photon generator at the center of a spaceship. When the generator is on, photons from it energize the whole craft to high \(a_{\psi\,n}\). When the generator is suddenly switched off, all the particles that constitute the craft relax to a lower energy state under a force field, \(B\) or \(E\), that is turned on as the generator is switched off. The craft is teleported.
But to which direction? In the case of a portal, the nature of \(t_c\) around \(x\) dictates that \(t_c\) slows down in a circular plane perpendicular to \(x\). Photons are inject from a circular perimeter clockwise, toward the center to slow time, \(t_c\) within the circle. The direction of travel is then into the circle, perpendicular to the plane of the circle.
In the case of a photon generator, the photons need be radiated outwards in a clockwise circular manner from stern to bow, then the spaceship will be driven forward.
The geometry of the photons, around the photon generator at the center, dictates the direction of travel.
Jump!