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Is the curvature index κ necessarily zero in a flat universe with cosmological constant?
The discussion revolves around the curvature index κ in the context of a flat universe with a cosmological constant. Participants explore the implications of the Friedmann-Robertson-Walker-Lemaitre models and the relationship between density parameters and curvature.
Participants express differing views on the relationship between curvature index and energy density, indicating that multiple competing perspectives remain unresolved regarding the implications of these definitions and conditions.
The discussion includes various assumptions about density parameters and their implications for curvature, which are not fully resolved. The definitions and relationships presented may depend on specific interpretations of cosmological models.
Yes. If a Friedmann-Robertson-Walker-Lemaitre universes has density (relative to critical density) ##1 = \Omega = \Omega_r + \Omega_r +\Omega_\Lambda##, then it is flat and ##\kappa = 0##. ("Flat" refers to spatial curvature (of 3-dimensional hypersurfaces), not to spacetime curvature.)Ranku said:Is the curvature index κ necessarily zero in a flat universe with cosmological constant?
To extend the discussion, the curvature index ##\kappa## can also cast in terms of its energy densityGeorge Jones said:Yes. If a Friedmann-Robertson-Walker-Lemaitre universes has density (relative to critical density) ##1 = \Omega = \Omega_r + \Omega_r +\Omega_\Lambda##, then it is flat and ##\kappa = 0##. ("Flat" refers to spatial curvature (of 3-dimensional hypersurfaces), not to spacetime curvature.)
No.Ranku said:To extend the discussion, the curvature index ##\kappa## can also cast in terms of its energy density
##\rho####\kappa#### =- \frac{3k}{8πGa^2}##. Can we identify the 'source' of ##\rho####\kappa##? Is it the matter density in the universe?