Abstract
The monopole mass can be substantially altered, in the string-like braneworld setup, and can be employed in order to constrain the brane thickness limit. In this work, we comprise a brief review regarding gauge fields localization in the string-like six dimensional braneworld models setup. The correction to the Coulomb's law in two models is studied. Besides, the monopole features are investigated from the point of view of the gauge fields localization in the string-like braneworlds, providing a more strict phenomenological bound for the braneworld thickness.
Highlights
The main aim of this work is to deal with the mass of the monopole, in string-like models on six dimensions
One can realize that the brane width for the Hamilton Cigar (HC) model, Eq (33), and for the GS model, Eq (36), are phenomenological bounds for the brane thickness into the 5th dimension, being respectively 3 and 2 orders of magnitude bigger than the theoretical bound of 2.0 × 10−19 m
The t’Hooft-Polyakov monopole radius and mass provided a phenomenological bound for the 6D brane thickness of the Gherghetta–Shaposhnikov and the Hamilton Cigar models
Summary
The main aim of this work is to deal with the mass of the monopole, in string-like models on six dimensions. It is remarkable to mention that in the scope of applications of brane-worlds models, several recent works perform the study of the informational entropy [1,2,3,4,5,6,7] underlying these scenarios, using Einstein-dilaton systems to derive phenomenologically compatible data. E., without the warp multiplicative factor, is dressed by the spontaneous symmetry breaking parameter in a Higgs-like potential, in a thick brane setup This radius is inversely proportional to the monopole mass [39]. The main concepts and results present in this paper are summarized in the concluding section IV
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