General Relativity - Riemann Tensor and Killing Vector Identity

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SUMMARY

The discussion focuses on deriving the identity V_{a;b;c}=V_eR^e_{cba} for a vector field V_a that satisfies the condition V_{a;b}+V_{b;a}=0. The key equations utilized include the Riemann tensor identity R^e_{abc}+R^e_{bca}+R^e_{cab}=0 and the second derivative identity V_{a;b;c}-V_{a;c;b}=V_eR^e_{abc}(0). The solution involves manipulating these identities to demonstrate the relationship between the derivatives of the vector field and the Riemann tensor.

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Homework Statement


I am trying to show that for a vector field Va which satisfies V_{a;b}+V_{b;a} that V_{a;b;c}=V_eR^e_{cba} using just the below identities.

Homework Equations



V_{a;b;c}-V_{a;c;b}=V_eR^e_{abc}(0)

R^e_{abc}+R^e_{bca}+R^e_{cab}=0 (*)

V_{a;b}+V_{b;a}=0 (**)

The Attempt at a Solution


So far I have:

V_eR^e_{cba}=-V_eR^e_{acb}-V_eR^e_{bac}=V_{a;b;c}-V_{a;c;b}+V_{b;c;a}-V_{b;a;c}=2V_{a;b;c}+V_{b;c;a}-V_{a;c;b}

Which gives:

V_eR^e_{cba}-V_{a;b;c}=V_eR^e_{abc}-V_{c;b;a}

I want to say that this implies V_{a;b;c}=V_eR^e_{cba} but I can't justify why both sides of the above equation must be zero. Can anyone see what else I can do? Thanks
 
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The problem is part of a larger question (see page 59 here http://www.maths.cam.ac.uk/undergrad/pastpapers/2004/Part_2/list_II.pdf ) and I'm having trouble with the last bit as well where it goes into the EM stuff, I know it must obviously somehow relate to everything we've done above but I just don't see the relevance.
 
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Can anybody help me out with deriving the identity <br /> V_{a;b;c}=V_eR^e_{cba}?<br />

Forget about the EM stuff I don't care so much about that but I'd be very grateful for some help in deriving that identity. Thanks
 
There's a couple of ways to show that. One way is to start from (*) and use (0) to write 6 terms involving the 2nd derivatives of the V's. Then you can use (**) to show that

V_{a;bc} + V_{b;ca} + V_{c;ab} =0.

You can then use (**) and (0) to show that

V_{b;ca} + V_{c;ab} = V_e {R^e}_{cab}.
 
fzero said:
There's a couple of ways to show that. One way is to start from (*) and use (0) to write 6 terms involving the 2nd derivatives of the V's. Then you can use (**) to show that

V_{a;bc} + V_{b;ca} + V_{c;ab} =0.

You can then use (**) and (0) to show that

V_{b;ca} + V_{c;ab} = V_e {R^e}_{cab}.

Ahhh thanks, done it now. It seems I was definitely going about it the wrong way.
 

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