Abstract
In the preceding paper, covariant and gauge-invariant quantities were defined that characterize density inhomogeneities in an almost-uniform model universe in a transparent way. In this paper second-order propagation equations are derived for these quantities in the case of a general "perfect fluid," and their properties examined. We do not use a harmonic decomposition in our definitions, but when such a decomposition is applied, our results are compatible with those obtained by Bardeen in his harmonically based gauge-invariant analysis. Our second-order equation enables a unified and transparent derivation of a series of results in the literature, without any ambiguity from choice of any particular gauge.
| Original language | English |
|---|---|
| Pages (from-to) | 1819-1826 |
| Number of pages | 8 |
| Journal | Physical Review D |
| Volume | 40 |
| Issue number | 6 |
| DOIs | |
| Publication status | Published - 15 Sept 1989 |