Monday, 07/24: Writing a pm-code - AIP
Monday, 07/24: Writing a pm-code - AIP
Monday, 07/24: Writing a pm-code - AIP
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Model equations 17<br />
It is also convenient to choose the expansion factor as time variable (using<br />
expressions for the Hubble constant: ȧ = aH(a)). For this choice of variables,<br />
the Poisson equation and equations of motion can be re-written as<br />
∇ 2 φ = 4πGΩ m,0 ρ crit,0 a −1 δ,<br />
δ = ρ − ¯ρ<br />
¯ρ ,<br />
dp<br />
da = −∇φ ȧ ,<br />
dx<br />
da =<br />
p<br />
ȧa 2.<br />
where δ is the overdensity in comoving coordinates and ȧ is<br />
ȧ = H 0 a −1/2 √Ω m,0 + Ω k,0 a + Ω Λ,0 a 3 ; Ω m,0 + Ω Λ,0 + Ω k,0 = 1