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Cosmology Cosmological solutions of
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Cosmology Cosmological solutions of
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Cosmology claimed to represent the
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Cosmology claimed to represent the
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Cosmology claimed to represent the
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Cosmology A) Empty Worlds, vacuum e
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Cosmology A) Empty Worlds, vacuum e
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Cosmology The general solution is S
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Cosmology The general solution is S
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Cosmology The general solution is S
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Cosmology (d) Λ > 0 , k = 0: S = e
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Cosmology (d) Λ > 0 , k = 0: S = e
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Cosmology (d) Λ > 0 , k = 0: S = e
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Cosmology Terminology: Λ > 0 , k =
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Cosmology Terminology: Λ > 0 , k =
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Cosmology Terminology: Λ > 0 , k =
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Cosmology B) Matter dominated: ρ >
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Cosmology B) Matter dominated: ρ >
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Cosmology ct = C arcsin √ X −
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Cosmology ct = C arcsin √ X −
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Cosmology ct = C arcsin √ X −
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Cosmology In each case we have S (t
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Cosmology In each case we have S (t
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Cosmology In each case we have S (t
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Cosmology Einstein-de Sitter univer
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Cosmology Einstein-de Sitter univer
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Cosmology t = 2 3 H−1 (t) (EdS) H
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Cosmology t = 2 3 H−1 (t) (EdS) H
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Cosmology Back to the non-flat geom
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Cosmology Back to the non-flat geom
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Cosmology in terms of the observabl
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Cosmology in terms of the observabl
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Cosmology in terms of the observabl
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Cosmology in terms of the observabl
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Cosmology The conclusion of the abo
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Cosmology The conclusion of the abo
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Cosmology The conclusion of the abo
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Cosmology C) Radiation dominated: p
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Cosmology C) Radiation dominated: p
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Cosmology C) Radiation dominated: p
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Cosmology ❖ k = 0 : S (t) = 4 ¯
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Cosmology In each case we have S (t
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Cosmology In each case we have S (t
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Cosmology In each case we have S (t
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Cosmology κ ρ(t) = 3 H2 (t) K(t)
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Cosmology Actually, in the radiatio
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Cosmology Actually, in the radiatio
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Cosmology 8π hν ργ(ν) dν = 3
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Cosmology 8π hν ργ(ν) dν = 3
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Cosmology Since ρ(t)S (t) 4 = ρ0S
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Cosmology c○ 2009, F. Jegerlehner
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Cosmology and Dicke and Peebles at
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Cosmology T0 = (2.725 ± 0.002) ◦
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Cosmology T0 = (2.725 ± 0.002) ◦
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Cosmology However, the evolution of
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Cosmology However, the evolution of
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Cosmology ρ(t) Big Bang radiation
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Cosmology The critical energy densi
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Cosmology The critical energy densi
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Cosmology The critical energy densi
- Page 121 and 122: Cosmology Ω0 = 1 c○ 2009, F. Je
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- Page 129 and 130: Cosmology ˙S 2 c 2 + k = κ 3 ρ S
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- Page 133 and 134: Cosmology q0 = κ (ρ0+3 p0) 6 H 2
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- Page 155 and 156: Cosmology Appendix: Λ 0 The issue
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