Why isn't the Cotton tensor identical zero?

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Cotton tensor C_{\mu\varkappa\lambda} is define as:
\nabla_{\sigma}W^{\sigma}_{\phantom{M}\mu\varkappa\lambda}=-\frac{n-3}{n-2}C_{\mu\varkappa\lambda}​
where W^{\sigma}_{\phantom{M}\mu\varkappa\lambda} is Weyl tensor and n is dimension of space.

Weyl tensor obey II. Bianchi identity (and all symetries of Rieamann tensor):
\nabla_{\nu}W^{\sigma}_{\phantom{M}\mu\varkappa\lambda} + \nabla_{\varkappa}W^{\sigma}_{\phantom{M}\mu\lambda\nu}+\nabla_{\lambda}W^{\sigma}_{\phantom{M}\mu\nu\varkappa}=0​
and extra it is traceless:
W^{\sigma}_{\phantom{M}\mu\sigma\varkappa}=0​
For a divergence of Weyl tensor can write:
\nabla_{\sigma}W^{\sigma}_{\phantom{M}\mu\varkappa\lambda}=g^{\rho\sigma}\nabla_{\sigma}W_{\rho\mu\varkappa\lambda}=\left<\mbox{II. Bianchi identity}\right>=-g^{\rho\sigma}\left(\nabla_{\varkappa}W_{\rho\mu\lambda\sigma}+\nabla_{\lambda}W_{\rho\mu\sigma\varkappa}\right)=
=\nabla_{\varkappa}W^{\sigma}_{\phantom{M}\mu\sigma\lambda}-\nabla_{\lambda}W^{\sigma}_{\phantom{M}\mu\sigma\varkappa}=0​
Becose Weyl tensor is traceless therefor Cotton tensor must be identical zero!
Is this correct?
 
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archipatelin said:
Cotton tensor C_{\mu\varkappa\lambda} is define as:
\nabla_{\sigma}W^{\sigma}_{\phantom{M}\mu\varkappa\lambda}=-\frac{n-3}{n-2}C_{\mu\varkappa\lambda}​
where W^{\sigma}_{\phantom{M}\mu\varkappa\lambda} is Weyl tensor and n is dimension of space.

Weyl tensor obey II. Bianchi identity (and all symetries of Rieamann tensor):
\nabla_{\nu}W^{\sigma}_{\phantom{M}\mu\varkappa\lambda} + \nabla_{\varkappa}W^{\sigma}_{\phantom{M}\mu\lambda\nu}+\nabla_{\lambda}W^{\sigma}_{\phantom{M}\mu\nu\varkappa}=0​
and extra it is traceless:
W^{\sigma}_{\phantom{M}\mu\sigma\varkappa}=0​
For a divergence of Weyl tensor can write:
\nabla_{\sigma}W^{\sigma}_{\phantom{M}\mu\varkappa\lambda}=g^{\rho\sigma}\nabla_{\sigma}W_{\rho\mu\varkappa\lambda}=\left<\mbox{II. Bianchi identity}\right>=-g^{\rho\sigma}\left(\nabla_{\varkappa}W_{\rho\mu\lambda\sigma}+\nabla_{\lambda}W_{\rho\mu\sigma\varkappa}\right)=
=\nabla_{\varkappa}W^{\sigma}_{\phantom{M}\mu\sigma\lambda}-\nabla_{\lambda}W^{\sigma}_{\phantom{M}\mu\sigma\varkappa}=0​
Becose Weyl tensor is traceless therefor Cotton tensor must be identical zero!
Is this correct?

Let's do clean the equations a little bit and see what's wrong:

From the second Bianchi Identity we have

\nabla_{\nu}W^{\sigma}_{\mu \varkappa \lambda}+\nabla_{\varkappa }W^{\sigma}_{\mu \lambda \nu}+\nabla_{\lambda }W^{\sigma}_{\mu \nu\varkappa}=0

Contracting \nu with \sigma gives

\nabla_{\sigma}W^{\sigma}_{\mu \varkappa \lambda}+\nabla_{\varkappa }W^{\sigma}_{\mu \lambda \sigma}+\nabla_{\lambda }W^{\sigma}_{\mu \sigma\varkappa}=0\Rightarrow

\nabla_{\sigma}W^{\sigma}_{\mu \varkappa \lambda}+\nabla_{\varkappa }W^{\sigma}_{\mu \lambda \sigma}-\nabla_{\lambda }W^{\sigma}_{\mu \varkappa\sigma}=0\Rightarrow

\nabla_{\sigma}W^{\sigma}_{\mu \varkappa \lambda}+g^{\rho \sigma}\nabla_{\varkappa }W_{\rho \mu \lambda \sigma}-g^{\rho \sigma}\nabla_{\lambda }W_{\rho \mu \varkappa\sigma}=0. (1)

Now I think by the property of tracelessness of Weyl tensor, or,

g^{\rho \sigma}W_{\rho \mu \varkappa\sigma}=0,

you conclude from (1)

\nabla_{\sigma}W^{\sigma}_{\mu \varkappa \lambda}=0.

So you put this into the equation

\nabla_{\sigma}W^{\sigma}_{\phantom{M}\mu\varkappa \lambda}=\frac{n-3}{n-2}C_{\mu\varkappa\lambda}

and finally claim that the Cotton tensor vanishes. But unfortunately you did make a big mistake. I let you think about where this flaw arises in the above calculations! You can have a look at the fact that in a geodesic coordinates, for example, the second derivatives of metric tensors wrt coordinates do not vanish whereas their first derevatives do.

AB
 
Altabeh said:
But unfortunately you did make a big mistake.
If do you think case when n=3. Yes, I did a big mistake. But I suppose n\geq4.
Or Cotton tensor exist only for n=3 space (for n=2 it is also zero)?
 
archipatelin said:
If do you think case when n=3. Yes, I did a big mistake. But I suppose n\geq4.
Or Cotton tensor exist only for n=3 space (for n=2 it is also zero)?

For n=3, the Cotton tensor does not vanish in general. But for n\geq4, if the weyl tensor vanishes, then the Cotton tensor always vanishes. For n less than 3 the Cotton tensor is not defined.

AB
 
Altabeh said:
For n=3, the Cotton tensor does not vanish in general. But for n\geq4, if the weyl tensor vanishes, then the Cotton tensor always vanishes. For n less than 3 the Cotton tensor is not defined.

AB

This is correct, because I made another big mistake. Weyl tensor isn't governed of analog II. Bianchi identity. Therefore cotton tensor is non-zero generaly for n>2.
 
Last edited:
archipatelin said:
This is correct, because I made another big mistake. Weyl tensor isn't governed of analog II. Bianchi identity. Therefore cotton tensor is non-zero generaly for n>2.

Seconded.
 
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