The linearization of the metric of curved space-time

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The discussion revolves around the linearization of the metric of curved space-time, specifically addressing the expression Yab=Xab-kHab+k2HacHcb. The participants clarify that the second-order term in k is HacHcb rather than Haccb due to the matrix identity (I + H)-1 = I - H + HH. There is confusion regarding the calculation of (HH)ab and the absence of the factor 1/2 in the Taylor series expansion of κ compared to that of H. The conversation emphasizes that the expansions of the metrics are similar due to their tensor rank. Overall, the participants are working to reconcile the differences in the expansions and clarify the mathematical relationships involved.
maica
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Why Yab=Xab-kHab+k2HacHcb-... and not Yab=Xab-kHab+(1/2)k2Haccb-...?
Y is the curved space-time metric
X is the planespace-time metric
 
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The second order term in k is HacHcb and not Haccb
 
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Because of the matrix identity (I + H)-1 = I - H + HH - ...
 
but this expansion is not an expansion matrix. these objects are components, numbers
 
maica said:
but this expansion is not an expansion matrix. these objects are components, numbers

How do you calculate the value of (HH)ab, given the components of H?
 
I'm a little lost. The expression (I+H)-1 = I - H + HH - ... is the Taylor series in powers of "H", but gij = ηij + κhij + (1/2)κ2hilhlj, is a series in powers of "κ", and doesn't have the expoent "-1", which is responsible for the absence of the factor 1/2 in the Taylor series of "H". I can't see why the factor 1/2 is absent, in Taylor series of "κ" powers. I think that the expansion of (HH)ab is identical of the gij expansion, because of de tensor rank.
 
I think that I understood. If we consider the equation gikgkj = δij and if gkj = ηkj + κ hkj then gik is the inverse and its expansion is gik = ηik - κ hik + κ2 hil hlk - ... identical to the expression (I + H)-1.
 
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