Bianchi and Ricci Identities: Understanding and Applying in Tensor Calculus

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Homework Statement
To prove ##{\nabla_a R_{bcd}}^a + \nabla_b R_{cd} - \nabla_c R_{bd}##
Relevant Equations
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Start with the Bianchi identity,$${\nabla_{[a} R_{bc]d}}^e = 0$$$${\nabla_{a} R_{bcd}}^e - {\nabla_{a} R_{cbd}}^e + {\nabla_{b} R_{cad}}^e - {\nabla_{b} R_{acd}}^e + {\nabla_{c} R_{abd}}^e - {\nabla_{c} R_{bad}}^e = 0$$Use definition of Ricci tensor$$

\left[ {\nabla_{a} R_{bcd}}^e + \nabla_b R_{cd} - \nabla_c R_{bd} \right] + \left[ {\nabla_c R_{abd}}^e - {\nabla_a R_{cbd}}^e - {\nabla_b R_{acd}}^e \right] = 0

$$How to proceed from here? Thanks
 
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etotheipi said:
$${\nabla_{a} R_{bcd}}^e - {\nabla_{a} R_{cbd}}^e + {\nabla_{b} R_{cad}}^e - {\nabla_{b} R_{acd}}^e + {\nabla_{c} R_{abd}}^e - {\nabla_{c} R_{bad}}^e = 0$$
You should be able to reduce the left side to just 3 terms by using the "skew symmetry" of the curvature tensor.

$$\left[ {\nabla_{a} R_{bcd}}^e + \nabla_b R_{cd} - \nabla_c R_{bd} \right] + \left[ {\nabla_c R_{abd}}^e - {\nabla_a R_{cbd}}^e - {\nabla_b R_{acd}}^e \right] = 0$$
You can see something's wrong here. Some of the terms have an index ##e## while other terms don't.
 
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Thanks! What about,$${\nabla_{a} R_{bcd}}^e - {\nabla_{a} R_{cbd}}^e + {\nabla_{b} R_{cad}}^e - {\nabla_{b} R_{acd}}^e + {\nabla_{c} R_{abd}}^e - {\nabla_{c} R_{bad}}^e = 0$$ $${\nabla_{a} R_{bcd}}^e + {\nabla_{b} R_{cad}}^e - {\nabla_{c} R_{bad}}^e = 0
$$Since ##a## and ##e## are free indices, we can choose to let ##a = e##, and sum over all ##a## [I'll write in the sum explicitly, and not use the convention here]$$\sum_a \left[ {\nabla_{a} R_{bcd}}^a + {\nabla_{b} R_{cad}}^a - {\nabla_{c} R_{bad}}^a \right] = 0$$Those final two terms we can contract over ##a##,$$\sum_a \left[ {\nabla_{a} R_{bcd}}^a \right] + \nabla_b R_{cd} - \nabla_c R_{bd} = 0$$
 
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for such problems it turns to be convenient to take into account that in a neighborhood of any point ##x'## there are local coordinates such that ##\Gamma_{ij}^k(x')=0##. This holds provided ##\Gamma_{ij}^k=\Gamma_{ji}^k##
 
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etotheipi said:
Thanks! What about,$${\nabla_{a} R_{bcd}}^e - {\nabla_{a} R_{cbd}}^e + {\nabla_{b} R_{cad}}^e - {\nabla_{b} R_{acd}}^e + {\nabla_{c} R_{abd}}^e - {\nabla_{c} R_{bad}}^e = 0$$ $${\nabla_{a} R_{bcd}}^e + {\nabla_{b} R_{cad}}^e - {\nabla_{c} R_{bad}}^e = 0
$$Since ##a## and ##e## are free indices, we can choose to let ##a = e##, and sum over all ##a## [I'll write in the sum explicitly, and not use the convention here]$$\sum_a \left[ {\nabla_{a} R_{bcd}}^a + {\nabla_{b} R_{cad}}^a - {\nabla_{c} R_{bad}}^a \right] = 0$$Those final two terms we can contract over ##a##,$$\sum_a \left[ {\nabla_{a} R_{bcd}}^a \right] + \nabla_b R_{cd} - \nabla_c R_{bd} = 0$$
Looks good to me
 
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