General relativity and the U(1) gauge group
Jean Paul Mbelek

TL;DR
This paper proposes a novel framework where gravity emerges from a U(1) gauge field, modeling the graviton as a bound state of gamma bosons, and formalizes gravity as a Yang-Mills theory without the need for a Higgs mechanism.
Contribution
It introduces a new model where gravity is derived from a U(1) gauge field, with the graviton as a bound state of gamma bosons, eliminating the need for symmetry breaking or Yukawa couplings.
Findings
Derivation of Einstein-like equations for gamma bosons
Static solutions reproduce Schwarzschild metric
Potential deviations from Schwarzschild solution testable experimentally
Abstract
We show that gravity together with curved spacetime can emerge, at the microscopic scale, from a U(1) gauge field. The gauge boson that carries gravity, of elementary particles, is proved to be a spin one massless and electrically neutral vector particle dubbed the "gamma boson" referring to the Dirac matrices, gamma_mu, which are promoted to be the quantum field for gravity at the scale of elementary particles. Instead, the graviton appears merely as a tensor bound state of two gamma bosons in the same spin eigenstate, by referring to the relation g_mu nu = 1/2 (gamma_mu gamma_nu + gamma_nu gamma_mu) and the metric ds^2 = g_mu nu dx^mu dx^nu = (gamma_alpha dx^alpha)^2. Consequently, like the electroweak theory and quantum chromodynamics, gravity may be formalized as a Yang-Mills theory. As a consequence, there is no need of the Higgs field or any symmetry breaking mechanism to generate…
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Taxonomy
TopicsCosmology and Gravitation Theories · Relativity and Gravitational Theory · Noncommutative and Quantum Gravity Theories
