Covariant derivative of Ricci scalar causing me grief

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Discussion Overview

The discussion revolves around the covariant derivative of the Ricci scalar and its relationship to the Bianchi identity. Participants explore the mathematical steps involved in deriving these relationships, focusing on potential mistakes in index manipulation and the implications of the Bianchi identity in the context of general relativity.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant expresses confusion about the covariant derivative of the Ricci scalar and its disagreement with the Bianchi identity, presenting their calculations.
  • Another participant points out a potential mistake in index contraction, suggesting that the participant is contracting the wrong indices.
  • A subsequent reply reiterates the concern about index contraction and proposes an alternative approach to the covariant derivative, indicating that the Bianchi identity may need to be indexed correctly.
  • Another participant suggests that the Bianchi identity should be expressed with indexed derivative operators, which may clarify the relationship between the Ricci tensor and the Ricci scalar.
  • Further clarification is provided regarding the correct form of the Bianchi identity and how it relates to the covariant derivative, emphasizing the importance of maintaining consistent indices throughout the derivation.

Areas of Agreement / Disagreement

Participants do not reach a consensus, as multiple competing views and interpretations of the mathematical steps remain. There is ongoing debate about the correct application of indices and the implications for the Bianchi identity.

Contextual Notes

Limitations include potential misunderstandings of index notation and the assumptions underlying the application of the Bianchi identity. The discussion reflects the complexity of the mathematical framework involved.

ft_c
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Hi all

I'm having trouble understanding what I'm missing here. Basically, if I write the Ricci scalar as the contracted Ricci tensor, then take the covariant derivative, I get something that disagrees with the Bianchi identity:

\begin{align*}
R&=g^{\mu\nu}R_{\mu\nu}\\
\Rightarrow \nabla R&=\nabla(g^{\mu\nu}R_{\mu\nu})\\
&=\nabla(g^{\mu\nu})R_{\mu\nu}+g^{\mu\nu}\nabla(R_{\mu\nu})\\
&=g^{\mu\nu}\nabla(R_{\mu\nu})\\
g_{\mu\nu}\nabla R&=g_{\mu\nu}g^{\mu\nu}\nabla(R_{\mu\nu})\\
&=4\nabla(R_{\mu\nu})\\
\Rightarrow \nabla(R_{\mu\nu}-\tfrac{1}{4}g_{\mu\nu} R)&=0
\end{align*}
whereas the contracted Bianchi identity is
$$\nabla(R_{\mu\nu}-\tfrac{1}{2}g_{\mu\nu}R)=0$$

If anyone could let me know what's going wrong here that would be much appreciated! Thanks very much in advance
 
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You are multiplying with ##g_{\mu\nu}## when you already have ##\mu## and ##\nu## as dummy indices in your expression and then you are contracting the wrong ##\mu## and ##\nu##. This is a very common student mistake.
 
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Orodruin said:
You are multiplying with ##g_{\mu\nu}## when you already have ##\mu## and ##\nu## as dummy indices in your expression and then you are contracting the wrong ##\mu## and ##\nu##. This is a very common student mistake.
Thanks Orodruin! I've actually already tried with different indices already, and I got the same thing, maybe you can take a look?
First write
$$g_{\mu\nu}R=g_{\mu\nu}g^{\rho\sigma}R_{\rho\sigma}$$
Covariant derivative
\begin{align*}
\nabla(g_{\mu\nu}R)&=\nabla(g_{\mu\nu}g^{\rho\sigma}R_{\rho\sigma})\\
g_{\mu\nu}\nabla R&=g_{\mu\nu}g^{\rho\sigma}\nabla R_{\rho\sigma}
\end{align*}

But $$\nabla R_{\rho\sigma} = \tfrac{1}{2}g_{\rho\sigma}\nabla R$$ from the Bianchi identity, so

\begin{align*}
g_{\mu\nu}\nabla R&=g_{\mu\nu}g^{\rho\sigma}(\tfrac{1}{2}g_{\rho\sigma}\nabla R)\\
&=\tfrac{1}{2}g_{\mu\nu}g^{\rho\sigma}g_{\rho\sigma}\nabla R\\
&=2g_{\mu\nu}\nabla R
\end{align*}

Can you see what's going wrong here? Thanks!
 
I'm just an amateur at this stuff, but maybe you need to index your derivative operator? So the second Bianchi identity ends up looking like:
$$\nabla^{a} (R_{ab} - \frac{1}{2}Rg_{ab}) = 0$$
or
$$\nabla_{a} (R^{ab} - \frac{1}{2}Rg^{ab}) = 0$$
 
So in post #3 above, the Bianchi identity should read:
$$\nabla^{\rho} R_{\rho\sigma} = \tfrac{1}{2}g_{\rho\sigma}\nabla^{\rho} R$$
but the covariant derivative line will read:
$$g_{\mu\nu}\nabla^{\mu} R=g_{\mu\nu}g^{\rho\sigma}\nabla^{\mu} R_{\rho\sigma}$$
or at least something where the index on ##\nabla## is not ##\rho##. So the pattern of indices doesn't allow for the substitution you made in that post. Instead, you'll get:
$$2\nabla^{\mu} R_{\mu\nu} =g_{\mu\nu}g^{\rho\sigma}\nabla^{\mu} R_{\rho\sigma} = \nabla^{\mu}Rg_{\mu\nu}$$
which is just the Bianchi identity again.
 
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