Cosmological redshift and nonlinear electrodynamics propagation of photons from distant sources
| dc.creator | Cuesta, Herman J. Mosquera | |
| dc.creator | Salim, Jose M. | |
| dc.creator | Novello, M. | |
| dc.date | 2007-10-26 | |
| dc.date.accessioned | 2026-07-07T08:39:04Z | |
| dc.date.available | 2026-07-07T08:39:04Z | |
| dc.description | By-now photons are the unique universal messengers. Cosmological sources like far-away galaxies or quasars are well-known light-emitters. Here we demonstrate that the nonlinear electrodynamics (NLED) description of photon propagation through the weak background intergalactic magnetic fields modifies in a fundamental way the cosmological redshift that a direct computation within a specific cosmological model can abscribe to a distant source. Independently of the class of NLED Lagrangian, the effective redshift turns out to be $1 + \tilde{z} = (1 + z) Δ$, where $Δ\equiv (1 + Φ_e)/(1 + Φ_o)$, with $Φ\equiv {8}/{3} ({L_{FF}}/{L_F}) B^2$, being $L_F = {dL}/{dF}$, $L_{FF} = {d^2L}/{dF^2}$, the field $F\equiv F_{αβ} F^{αβ}$, and $B$ the magnetic field strength. Thus the effective redshift is always much higher then the standard redshift, but recovers such limit when the NLED correction $Δ(Φ_e, Φ_o) \longrightarrow 1$. This result may provide a physical foundation for the current observation-inspired interpretation that the universe undergoes an accelerate expansion. However, under the situation analyzed here, for any NLED the actual (spatial) position of the light-emitting far-away source remains untouched. | |
| dc.description | 5 pages, 3 figures, revtex4.sty | |
| dc.identifier | https://arxiv.org/abs/0710.5188 | |
| dc.identifier | http://arxiv.org/abs/0710.5188 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/140949 | |
| dc.subject | Astrophysics | |
| dc.title | Cosmological redshift and nonlinear electrodynamics propagation of photons from distant sources | |
| dc.type | text |