Dark-Energy Dynamics Required to Solve the Cosmic Coincidence
| dc.creator | Egan, Chas A. | |
| dc.creator | Lineweaver, Charles H. | |
| dc.date | 2007-12-19 | |
| dc.date | 2008-10-14 | |
| dc.date.accessioned | 2026-07-07T11:54:45Z | |
| dc.date.available | 2026-07-07T11:54:45Z | |
| dc.description | Dynamic dark energy (DDE) models are often designed to solve the cosmic coincidence (why, just now, is the dark energy density $ρ_{de}$, the same order of magnitude as the matter density $ρ_m$?) by guaranteeing $ρ_{de} \sim ρ_m$ for significant fractions of the age of the universe. This typically entails ad-hoc tracking or oscillatory behaviour in the model. However, such behaviour is neither sufficient nor necessary to solve the coincidence problem. What must be shown is that a significant fraction of observers see $ρ_{de} \sim ρ_m$. Precisely when, and for how long, must a DDE model have $ρ_{de} \sim ρ_{m}$ in order to solve the coincidence? We explore the coincidence problem in dynamic dark energy models using the temporal distribution of terrestrial-planet-bound observers. We find that any dark energy model fitting current observational constraints on $ρ_{de}$ and the equation of state parameters $w_0$ and $w_a$, does have $ρ_{de} \sim ρ_m$ for a large fraction of observers in the universe. This demotivates DDE models specifically designed to solve the coincidence using long or repeated periods of $ρ_{de} \sim ρ_m$. | |
| dc.description | 16 pages, 8 figures, Submitted to Phys. Rev. D | |
| dc.identifier | https://arxiv.org/abs/0712.3099 | |
| dc.identifier | http://arxiv.org/abs/0712.3099 | |
| dc.identifier | Phys.Rev.D78:083528,2008 | |
| dc.identifier | doi:10.1103/PhysRevD.78.083528 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/205017 | |
| dc.subject | Astrophysics | |
| dc.title | Dark-Energy Dynamics Required to Solve the Cosmic Coincidence | |
| dc.type | text |