General Relativity - Riemann Tensor and Killing Vector Identity

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Homework Help Overview

The discussion revolves around demonstrating an identity involving the Riemann tensor and a vector field in the context of general relativity. The original poster is attempting to show that for a vector field \( V_a \) satisfying a specific condition, the relation \( V_{a;b;c} = V_e R^e_{cba} \) holds, using given identities and equations.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to manipulate the provided identities to derive the desired relation but struggles to justify certain steps. Some participants suggest starting from established identities and using them to derive additional relationships involving the second derivatives of the vector field.

Discussion Status

Participants are exploring various methods to derive the identity, with some providing guidance on how to approach the problem using the given equations. There is an acknowledgment of different ways to arrive at the conclusion, but no explicit consensus is reached regarding the best method.

Contextual Notes

The problem is part of a larger question that includes additional context related to electromagnetic theory, which some participants note as potentially relevant but not central to their current focus.

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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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