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Cosmological solutions of the Einstein-Friedmann equations ...

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Cosmology<br />

T0 = (2.725 ± 0.002) ◦ K<br />

not only clearly favored Big-Bang cosmologies and essentially ruled out<br />

steady-state <strong>the</strong>ory, it by now provides <strong>the</strong> best test <strong>of</strong> isotropy at <strong>the</strong> level <strong>of</strong> 0.1%<br />

over 360 ◦ <strong>of</strong> <strong>the</strong> sky! We will come to that later.<br />

What does it mean? First we have<br />

ρ0γ = a T 4 0 c2 ✄ ρ0γ 4.64 × 10 −34 gr/cm 3 × c 2 , n0γ 410 photons/cm 3<br />

which confronts with <strong>the</strong> present baryonic matter density<br />

ρ0,mat 3 × 10 −31 gr/cm 3 × c 2 .<br />

c○ 2009, F. Jegerlehner ≪❘ Lect. 7 ❘≫ 467

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