Variation of the metric tensor determinant

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The discussion focuses on the variation of the determinant of the metric tensor, expressed as δ(det[gμν]). The key equation derived is δ(det[gμν]) = det[gμν] Tr(gμν⁻¹ δ[gμν]). Participants explore the challenges of removing the trace and maintaining clarity in matrix multiplication. A more refined approach suggests that δ(det(g)) can be simplified to involve the trace of the product of the metric tensor and its variation. The conversation also touches on LaTeX formatting tips for clearer mathematical expression.
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Homework Statement



This is not homework but more like self-study - thought I'd post it here anyway.

I'm taking the variation of the determinant of the metric tensor:

\delta(det[g<sub>\mu</sub><sub>\nu</sub>]).


Homework Equations



The answer is

\delta(det[g<sub>\mu\nu</sub>]) =det[g\mu\nu] g\mu\nu \deltag\mu\nu

Here, g\mu\nu is the metric tensor, [g\mu\nu] is the matrix of the components of the metric tensor, and \delta is a variation.


The Attempt at a Solution



I have managed to get close to the answer, I hope, with
\delta(det[g<sub>\mu\nu</sub>])
=det[g\mu\nu] tr([g\mu\nu]-1\delta([g\mu\nu]))

The problem, in my view, is the trace. I cannot see how to remove it.

Also, if someone could kindly describe how to tidy the LaTeX up, I will do that.

Thank you!
 
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You can't use the tags in latex. Instead, write g_{\mu \nu}, g^{\mu \nu} etc.

InsertName said:
I have managed to get close to the answer, I hope, with
\delta(\det[g_{\mu\nu}]) = \det[g_{\mu\nu}] \mathrm{Tr}([g_{\mu\nu}^{-1}\delta([g_ {\mu\nu}]))

This is a little bit tricky, as you don't really keep track of how your matrices are multiplied together. If you do it with more care, you should find something like
\delta \det(g) = \det(g) \mathrm{Tr}( g \cdot \delta(g) ),
with (g \cdot \delta(g))_{\mu \nu} = g_{\mu \lambda} \delta ({g^\lambda}_\nu)
Now it's easy to see what the trace is:
\mathrm{Tr}( g \cdot \delta(g) ) = (g \cdot {\delta(g))_\mu}^{\mu} = g_{\mu \lambda} \delta (g^{\lambda \mu})
 
use
g=(1/4!)εαβγδεμvρσgαμgβvgγρgδσ
ggαμαβγδεμvρσgβvgγρgδσ
now when you apply δ on g you can use the second of the above to get whole result.(i am not going to do it in full,because of the requirement of homework section)
 
Hmm,may be tough.
so use Tr (ln M)=ln(det M)
variation of it yields,
Tr(M-1 δM)=(1/det M)δ(det M)
JUST PUT M=gμv
 

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