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Cosmological solutions of the Einstein-Friedmann equations ...

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Cosmology<br />

<strong>Cosmological</strong> <strong>solutions</strong> <strong>of</strong> <strong>the</strong> <strong>Einstein</strong>-<strong>Friedmann</strong> <strong>equations</strong><br />

Summary <strong>of</strong> <strong>Friedmann</strong>’s <strong>equations</strong><br />

Ingredients are <strong>the</strong> <strong>Einstein</strong> <strong>equations</strong> <strong>of</strong> GRT:<br />

Rµν − 1<br />

2 R gµν − Λ gµν = κ Tµν ,<br />

with <strong>the</strong> cosmic ideal fluid energy-momentum tensor<br />

T µν = (ρ + p) (t) u µ u ν − p(t) g µν .<br />

The cosmological constant term Λ gµν nowadays is usually included as part <strong>of</strong> Tµν<br />

as an additional contribution to <strong>the</strong> energy density<br />

ρ(t) → ρ(t) + ρΛ ; ρΛ = Λ<br />

κ ,<br />

c○ 2009, F. Jegerlehner ≪❘ Lect. 7 ❘≫ 439

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