Light motion as a bandwidth adapted aggregate

I thought that light should move even if no one was looking and there was no time or space. So, li8ght has to move via the adaptation process, a process trying to match exchange rates between a bundle of hot positions and the density of cold positions in the vacuum; using terminology from the game of Wythoff.

Fake Chart

So, I made a fake power spectrum, using the distribution of Coth and Tanh, derived from their second derivatives.  Coth are cold positions, they  exchange at half the rate of the hot positions. Cold in red, hot in blue; and they look like fermion and boson statistics.

Now in this model, the vacuum of space has cold positions, but when a density of hot positions are dumped into the vacuum, the bandwidth equalization process takes over.  Cold positions are redistributed such that their probability is four times the probability of the hot positions. In the chart I did this by shifting X and 1/X exponent to simulate charge. But since the probability distributions of fermion and boson are asymmetric, there will not be a complete match. At some point the cold positions will have more bandwidth than the hot. That point is the line of symmetry over which the hot positions will move.  Other hot positions, with high quant, greater exchange rate, will circle back.

I am close here, but I am in no position to try out actual numbers.  However, I am almost certain that this is the method used when the modern physicist dumps time and distance.