Paper
Whole Gauge Physicality
- Authors:
- J. Chauca; R. Doria
- Abstract
- Considering that nature also has a systemic behaviour, there is still space for a whole physics to be derived from gauge symmetry. Therefore, by observing such nature systemic behaviour, a systemic symmetry is introduced. It originates the so-called whole gauge theory. It is a model based on the meaning that to a given Lorentz group representation should be associated with a field family. So, given the representation {□(1/2),□(1/2)}, it provides a dynamics with N-potential fields rotating under a same symmetry group. It develops a new possibility for gauge invariance to be explored which is to work as building maker of a group of fields. Thus, given that nature work as a group, one moves from the usual physics given by just one field G_μ to a physics where this field is inserted in a group 〖{G〗_μ^I}. New properties are developed. At this work, one studies on such new features which are the fields non-linearity, granular and collective, connectivity, global interactivity, directive and circumstance, gauge organization, complexity. Our framework for this investigation is the abelian fields set {G_μ^I}. By analyzing the corresponding gauge invariant Lagrangian these new properties are deducted. They are showing a new physicality for the quanta. They are consequence from the parts to be enfolded in the whole given by the Lorentz group representation.
- Keywords
- Whole Abelian Model; Non-linearity; Connectivity; Gauge Organization; Complexity
- StartPage
- 253
- EndPage
- 264
- Doi