2012
DOI: 10.1016/j.amc.2012.07.035
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On asymptotic solutions of Friedmann equations

Abstract: Our main aim is to apply the theory of regularly varying functions to the asymptotical analysis at infinity of solutions of Friedmann cosmological equations. A new constant Γ is introduced related to the Friedmann cosmological equations. Determining the values of Γ we obtain the asymptotical behavior of the solutions, i.e. of the expansion scale factor a(t) of a universe. The instance Γ < 1 4 is appropriate for both cases, the spatially flat and open universe, and gives a sufficient and necessary condition for… Show more

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Cited by 3 publications
(16 citation statements)
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“…The significance of the integral limit (1.14) is seen in the following facts. We have shown in Mijajlović et al [27] that for any function µ ∈ M such that Γ µ < 1/4, the Friedmann equations has a normalized regularly varying solutions and the universe modelled by these solutions must be spatially flat or open. On the other hand, if Γ µ > 1/4 then the universe is oscillatory.…”
Section: The Constant γmentioning
confidence: 93%
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“…The significance of the integral limit (1.14) is seen in the following facts. We have shown in Mijajlović et al [27] that for any function µ ∈ M such that Γ µ < 1/4, the Friedmann equations has a normalized regularly varying solutions and the universe modelled by these solutions must be spatially flat or open. On the other hand, if Γ µ > 1/4 then the universe is oscillatory.…”
Section: The Constant γmentioning
confidence: 93%
“…The function M(µ) is a linear functional M : M → R, where M is the space of all real functions satisfying the above integral condition (1.14). M is called a Marić class of functions (see Mijajlović et al [27]). If this integral limit does not exist, we say that Γ does not exist.…”
Section: The Constant γmentioning
confidence: 99%
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