Deriving FRW Metric: Ricci Vector Algebra Explained

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SUMMARY

The discussion focuses on deriving the Friedmann-Robertson-Walker (FRW) metric using Ricci vector algebra as outlined in the paper "http://arxiv.org/pdf/gr-qc/9712019.pdf". Participants clarify that by setting ##\partial_{0} \beta## and ##\alpha=0##, the Christoffel symbols and Riemann tensors with a ##0## index vanish, leaving only Ricci vectors with indices ##1, 2, 3##. The metric's time dependence is factored out, leading to the conclusion that the coefficient of ##dt^{2}## becomes ##-1##, as shown in equation 8.1, allowing for the spatial metric to be expressed in terms of the scale factor ##a(t)## and the function ##\gamma_{ij}##.

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binbagsss
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I'm looking at: http://arxiv.org/pdf/gr-qc/9712019.pdf,

deriving the FRW metric, and I don't fully understand how the Ricci Vectors eq 8.5 can be attained from 7.16, by setting ##\partial_{0} \beta ## and ##\alpha=0##

I see that any christoffel symbol with a ##0## vanish and so so do any Riemann tensors with a ##0##, and so only Ricci vectors with ##1,2,3## indices will be non-zero

However, I thought the metric used to compute the Ricci vectors in eq 7.16 - 7.13- would need to reduce to 8.4.
So I see ##\beta(t,r) -> \beta(t) ##, but I thought also the ##dt^{2}## coefficient would also have to vanish?

Thanks in advance.
 
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binbagsss said:
I thought the metric used to compute the Ricci vectors in eq 7.16 - 7.13- would need to reduce to 8.4.

It does. But that portion of the metric is only the spatial portion, with the ##t## dependence already factored out. See below.

binbagsss said:
I see ##\beta(t,r) -> \beta(t)## ,

I think you mean ##\beta(r)##, correct? In equation 8.4, ##\beta## is a function of ##r## only; the ##t## dependence was already factored out in equation 8.1. See below.

binbagsss said:
I thought also the ##dt^{2}## coefficient would also have to vanish?

Setting ##\alpha = 0## means the coefficient of ##dt^2##, which is ##- e^{2 \alpha}##, becomes ##-1##. That's what is shown in equation 8.1, which also factors out the ##t## dependence of the spatial part of the metric into the scale factor ##a(t)##. Equation 8.4 is then just an equation for what's left in the spatial part in 8.1, i.e., the function ##\gamma_{ij}##.
 

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