Contracting R_{αβ} to R^ρ_αβσ: No 16 Multiplier

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SUMMARY

The discussion focuses on the contraction of the Riemann curvature tensor \( R_{\alpha \beta} \) to \( R^{\rho}_{\alpha\beta\sigma} \) without the application of a multiplier, specifically avoiding the factor of 16 associated with \( g^{\rho\xi}g_{\xi\sigma} \). Participants clarify that \( g^{\rho\xi}g_{\xi\sigma} \) simplifies to \( \delta^\rho_\sigma \), leading to the conclusion that \( g^{\sigma\xi}g_{\xi\rho} R^{\rho}{}_{\alpha\beta\sigma} \) equals \( \delta^\sigma_\rho R^{\rho}{}_{\alpha\beta\sigma} \), which ultimately results in \( R^{\sigma}{}_{\alpha\beta\sigma} \). The use of the metric tensor \( \eta \) in cosmological space-times is deemed unnecessary.

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  • Familiarity with tensor contraction techniques
  • Knowledge of metric tensors, specifically \( g^{\rho\xi} \) and \( g_{\xi\sigma} \)
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pleasehelpmeno
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Can anyone explain how to contract R_{\alpha \beta} to R^{\rho}_{\alpha\beta\sigma} without multiplying it by 16 i.e g^{\rho\xi}g_{\xi\sigma} It is in a sum with other tensor products and so I obviusly can't just multiply one term by anything ither than 1.

Should \eta's be used although are these valid in cosmological space-times i.e dt^2 -a^2 dx^2

I apologise if any indices aren't in the correct order, I am self taught
 
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pleasehelpmeno said:
Can anyone explain how to contract R_{\alpha \beta} to R^{\rho}_{\alpha\beta\sigma} without multiplying it by 16 i.e g^{\rho\xi}g_{\xi\sigma} It is in a sum with other tensor products and so I obviusly can't just multiply one term by anything ither than 1.

g^{\rho\xi}g_{\xi\sigma} = \delta^\rho_\sigma not 16. Consequently,

g^{\sigma\xi}g_{\xi\rho} R^{\rho}{}_{\alpha\beta\sigma} = \delta^\sigma_\rho R^{\rho}{}_{\alpha\beta\sigma} = R^{\sigma}{}_{\alpha\beta\sigma}
pleasehelpmeno said:
Should \eta's be used

No.
 

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