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Linear cosmological density perturbation
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Words: 252
Articles: 12
For pressureless subhorizon matter perturbations, a Fourier mode in conformal time obeys
δ
′′
+
H
δ
′
−
2
3
Ω
M
H
2
δ
=
0
,
(26)
where
H
=
a
′
/
a
.
Table of contents
252
12
Density contrast
Linear cosmological density perturbation
25
1
Linearized cosmological continuity equation
Density contrast
16
Jeans wavenumber
Linear cosmological density perturbation
11
Radiation domination
Linear cosmological density perturbation
13
Matter-era growing and decaying density modes
Linear cosmological density perturbation
65
2
Cosmic-time matter density modes
Matter-era growing and decaying density modes
25
Matter-era linear growth factor
Matter-era growing and decaying density modes
17
Cosmological horizon crossing
Linear cosmological density perturbation
63
2
Horizon-crossing time across matter-radiation equality
Cosmological horizon crossing
18
Matter-era transfer of a horizon-crossing amplitude
Cosmological horizon crossing
24
Cosmological density power spectrum
Linear cosmological density perturbation
56
1
Broken matter power spectrum from horizon entry
Cosmological density power spectrum
28
Ancestors
(4)
Cosmology
Branch of physics
Physics
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