Charged Axially Symmetric Solution and Energy in Teleparallel Theory Equivalent to General Relativity
| dc.creator | Nashed, Gamal Gergess Lamee | |
| dc.date | 2007-06-02 | |
| dc.date.accessioned | 2026-07-07T10:36:01Z | |
| dc.date.available | 2026-07-07T10:36:01Z | |
| dc.description | An exact charged solution with axial symmetry is obtained in the teleparallel equivalent of general relativity (TEGR). The associated metric has the structure function $G(ξ)=1-ξ^2-2mAξ^3-q^2A^2ξ^4$. The fourth order nature of the structure function can make calculations cumbersome. Using a coordinate transformation we get a tetrad whose metric has the structure function in a factorisable form $(1-ξ^2)(1+r_{+}Aξ)(1+r_{-}Aξ)$ with $r_{\pm}$ as the horizons of Reissner-Nordstr$\ddot{o}$m space-time. This new form has the advantage that its roots are now trivial to write down. Then, we study the singularities of this space-time. Using another coordinate transformation, we obtain a tetrad field. Its associated metric yields the Reissner-Nordstr$\ddot{o}$m black hole. In Calculating the energy content of this tetrad field using the gravitational energy-momentum, we find that the resulting form depends on the radial coordinate! Using the regularized expression of the gravitational energy-momentum in the teleparallel equivalent of general relativity we get a consistent value for the energy. | |
| dc.description | 15 pages, Latex | |
| dc.identifier | https://arxiv.org/abs/0706.0260 | |
| dc.identifier | http://arxiv.org/abs/0706.0260 | |
| dc.identifier | Eur.Phys.J.C49:851-857,2007 | |
| dc.identifier | doi:10.1140/epjc/s10052-006-0154-x | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/179917 | |
| dc.subject | General Relativity and Quantum Cosmology | |
| dc.title | Charged Axially Symmetric Solution and Energy in Teleparallel Theory Equivalent to General Relativity | |
| dc.type | text |