Nature of the Curvature of Space-Time

At first sight, a graviton as the united gauge boson [1] may be described by a vector (axial-vector) field, but this is not quite so. The point is that the vectors (axial vectors) constitute the plane surface. The same corresponding individual force of a Newton or Coulomb nature does not influence

a given procedure, and consequently, the field of such an action remains linear. Unlike this, the electric, weak, and strong parts and other innate parts of gravitational force arise because of the harmony of a kind of Newton-Coulomb pair of forces. However, at the interratio of each Newton-Coulomb pair of intragraviton forces, their individual vectors (axial vectors) become naturally curved vectors (axial vectors), which constitute the curved surface. It is already clear from the foregoing that a curvature of space-time reflects the availability in it of the harmony of forces of a different nature. Therefore, an individual field of each of the gauge bosons must be considered

as the naturally curved field of the unified system of the two fields of the Coulomb and Newton behavior in which appears a part of the mass-charge structure of gauge invariance. This becomes

more interesting if we include in the discussion an interratio of intranuclear forces. Their harmony responds to the periodic revolution around the nucleus of any of the corresponding types of fermions of leptonic families [2]. At such a situation, the field of action of each of the structural components of the gravitational force between the nucleus and its satellite must be naturally

curved. As a consequence, each lepton with a linear velocity in an atom undergoes orbital

rather than straight-line motion.

[1] R.S. Sharafiddinov, Bull. Am. Phys. Soc. {f 60}, E13.00008 (2015).

[2] R.S. Sharafiddinov, Phys. Essays {f 34}, 3 (2021) 398.