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Hi does anyone know how to calculate:
\delta (det|g_{\mu\nu}|) or simply \delta g
\delta (det|g_{\mu\nu}|) or simply \delta g
The discussion centers on the calculation of the variation of the determinant of the metric tensor, specifically \(\delta (det|g_{\mu\nu}|)\) or \(\delta g\). The participants reference Jacobi's formula for derivatives of determinants and identify a sign error in the expression for \(\delta g_{\mu\nu}\). They clarify that the correct relationship is \(\delta g_{\mu\nu} = - g^{\alpha\mu} g^{\beta\nu} \delta g_{\alpha\beta}\), and provide a specific case using \(g_{\mu\nu} = \lambda \eta_{\mu\nu}\) to illustrate the sign discrepancies in the calculations.
PREREQUISITESThe discussion is beneficial for physicists, mathematicians, and students studying general relativity or differential geometry, particularly those working with metric tensors and their variations.
Actually I believe this answer has a sign error, and does not correspond to what I wrote, since δgμν = - gμα gνβ δgαβ.You should get δg=ggμνδ(gμν)
Bill_K said:Actually I believe this answer has a sign error, and does not correspond to what I wrote, since δgμν = - gμα gνβ δgαβ.
A quick way to check the sign is to consider a special case, gμν = λ ημν under the variation δλ. For this case,
gμν = λ-1 ημν and g = -λ4, so δgμν = ημν δλ and δg = -4 λ3 δλ.
The minus sign agrees with the expression I gave, namely g gμν δgμν = (-λ4)(λ-1ημν)(ημν δλ).
However the other expression g gμν δ(gμν) = (-λ4)(λ ημν)(-λ-2) (ημν δλ) comes out positive, which is incorrect.