Integral over 4D Metrics: Volume Element?

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SUMMARY

The discussion centers on determining the invariant volume element for a 4D integral of the form \(\int d^{10} \eta \delta (\eta - \bar \eta)\). The user proposes that the invariant volume element is \(\frac{d^{10} \eta}{J^2}\), where \(J\) represents the Jacobian. The logic presented involves the transformation of coordinates, specifically \(d\bar x^\alpha = \frac{\partial \bar x^\alpha}{\partial x^\beta}dx^\beta\) and the relationship between the determinants of the metrics, leading to the conclusion that \(d^{10} \bar g = \frac{d^{10} g}{J^2}\). The user also specifies conditions for the metric, including \(g_{00} < 0\) and the determinants of the metrics being positive or negative as required.

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  • Basic concepts of integrals in higher-dimensional spaces
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Jim Kata
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I'm going to be working in 4D, and I assume my metric is symmetric. So what I am interested in is an integral of the form [tex]\int {d^{10} \eta \delta (\eta - \bar \eta } )[/tex]. My question is what is the invariant volume element for an integral of this type? My guess is that it is [tex]\frac{{d^{10} \eta }}{{J^2 }}[/tex] where [tex]J[/tex] is the jacobian, but I don't know. This my logic:
[tex]d\bar x^\alpha = \frac{{\partial \bar x^\alpha }}{{\partial x^\beta }}dx^\beta[/tex] and [tex]d^4 \bar x = \frac{{d^4 x}}{J}[/tex]. So since:[tex]\bar g^{\alpha \beta } = g^{\mu \tau } \frac{{\partial \bar x^\alpha }}{{\partial x^\mu }}\frac{{\partial \bar x^\beta }}{{\partial x^\tau }}[/tex] I figured [tex]d^{10} \bar g = \frac{{d^{10} g}}{{J^2 }}[/tex]. I would also like the requirements that [tex]g_{00} < 0[/tex], [tex]\det [g_{\alpha \beta } ] < 0[/tex], and [tex]\det [\gamma _{ij} ] > 0[/tex] where [tex]\det [g_{\alpha \beta } ] = g_{00} \det [\gamma _{ij} ][/tex]. Any suggestions or guesses?
 
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Jim Kata said:
I'm going to be working in 4D, and I assume my metric is symmetric.

A metric, by definition, satisfies d(x,y)=d(y,x).
 

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