2022
DOI: 10.1007/s10714-022-02955-y
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Remarks on the cosmological constant appearing as an initial condition for Milne-like spacetimes

Abstract: Milne-like spacetimes are a class of $$k = -1$$ k = - 1 FLRW spacetimes which admit continuous spacetime extensions through the big bang. In a previous paper Ling (Found. of Phys. 50:385–428, 2020), it was shown that the cosmological constant appears as an initial condition for Milne-like spacetimes. In this paper, we generalize this statement to spacetimes which share similar … Show more

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Cited by 5 publications
(4 citation statements)
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“…Therefore, an important mathe-JHEP10(2023)182 matical question is to find examples of spacetimes satisfying the hypotheses of Theorem 5.2, which do not belong to the class of past-asymptotically de Sitter spacetimes. The same question remains in the Milne-like case as well [48].…”
Section: Discussion and Future Directionsmentioning
confidence: 91%
See 2 more Smart Citations
“…Therefore, an important mathe-JHEP10(2023)182 matical question is to find examples of spacetimes satisfying the hypotheses of Theorem 5.2, which do not belong to the class of past-asymptotically de Sitter spacetimes. The same question remains in the Milne-like case as well [48].…”
Section: Discussion and Future Directionsmentioning
confidence: 91%
“…Specifically, we will mostly explore spacetimes that are flat past-asymptotically dS and derive conditions on their extendibility. There will be many parallels with the works of [38,[46][47][48][49] on the topic of metric extendibility of Milne-like spacetimes, which are homogeneous and isotropic universes with negative (as opposed to zero here) constant spatial curvature.…”
Section: Jhep10(2023)182mentioning
confidence: 98%
See 1 more Smart Citation
“…Indeed in the dark energy case p = −ρ the above inequality is satisfied and the universe is accelerating. If this is taken as the correct equation of state near the inception of the universe this means that [8] we have ä > 0 at those early time, meaning that if we go back enough to some t c then ȧ(t c ) = 0, and the scale factor reaches a minimal finite size a c = a(t c ) and thus the singularity is avoided. However, this scenario is not plausible because ordinary matter density is expected to be much higher than dark energy density at those early times making the above accelerating scenario invalid.…”
Section: Implications Of the Flrw Equationsmentioning
confidence: 99%