Distances and renormalization


• As for durations, the notion of distance between two “points of space” risks to have no meaning in the absence of interaction.

If one tries to found upon the Feynman's style diagrams, one may propound to count the number N of intermediate nodes, and consider a distance of the form  d = ndelta  where delta is an elementary (arbitrary ?) distance.

This gives back in particular  N = 0  and  d = 0  for an isolated (naked) propagator, what is consistent with the relativistic instantaneousness here considered ; but within such a model, is the distance independent of the kind of interaction considered to foreseen it (the question arises as soon as one considers more complex diagrams) ?

Thus the following diagrams (with respect to the two outmost points) would correspond respectively to  N = 2,  N = 1  and  N = 2 or 3 (?).

masse1
masse2
masse3

Dimensionnal analysis furthermore allows to propound as elementary quantified distance the value  racine3 = 4,0.10-35 m  (sometimes called “Planck distance”, but this is not necessarily the appropriate value).

• Among the difficulties issued from the model, an important point is the necessary reinterpretation of the renormalization.

Within usual quantum theories, some diagrams with more branches occur as higher order corrections with respect to simpler diagrams describing the same interaction. In the argumentation considered here, these diagrams would occur in the description of the same phenomenon, but later (as with more branches).

This aspect which may look as troublesome is not necessarily “negative”, since if one consider that as the time proceeds, the “dressed up” propagator describing an interaction complexifies itself, and that this is connected to an increase of distances, thus this may lead to a “natural” effect of  Universe expansion.

• Inversely, in order to describe a “constant distance” between two points which interact “always likewise” (the two ends of a length standard ?), it might be necessary to introduce a renormalization of distances (the length standard is submitted to expansion in a similar way as the distances that it is supposed to measure).

The renormalization would thus be different : the mass would issue from “lateral” branches of diagrams (associated with undetected interactions), and not from “loops”, which on the contrary would intervene in a renormalization of distances.

• After that, it would be elsewere necessary to think to define clearly some notions as mouvement, and so on...



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