Calculating Covariant Derivative of Riemann Tensor in Riemann Normal Coordinates

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SUMMARY

The covariant derivative of the Riemann tensor, as presented in equation 3.86 of Carroll's lecture notes on general relativity, simplifies to a partial derivative when evaluated in Riemann normal coordinates. In these coordinates, the Christoffel symbols vanish at a specific point, allowing for this simplification. However, while the Christoffel symbols themselves vanish, their derivatives do not, which means the Riemann tensor does not vanish at that point. This distinction is crucial for understanding the behavior of tensors in general relativity.

PREREQUISITES
  • Understanding of Riemann normal coordinates
  • Familiarity with the Riemann tensor and its properties
  • Knowledge of Christoffel symbols and their role in general relativity
  • Basic grasp of covariant derivatives and their computation
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  • Study the derivation of the Riemann tensor in Riemann normal coordinates
  • Explore the implications of vanishing Christoffel symbols on tensor calculations
  • Learn about the significance of derivatives of Christoffel symbols in general relativity
  • Review advanced topics in differential geometry related to curvature and geodesics
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Covariant derivative of the Riemann tensor evaluated in Riemann normal coordinates
Hello everyone,

in equation 3.86 of this online version of Carroll´s lecture notes on general relativity (https://ned.ipac.caltech.edu/level5/March01/Carroll3/Carroll3.html) the covariant derviative of the Riemann tensor is simply given by the partial derivative, the terms carrying the Christoffel symbols seem to vanish. I assume this results from the note that it is evaluated in Riemann normal coordinates. I know one can choose the coordinate system so that a given Christoffel-symbol vanishes but in this case there are so many to handle so that I am not convinced this is working. Can someone please give me an input on how to make myself clear that it works? Thanks in advance!
 
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Can you be more specific. What doesn't seem to work? It looks perfectly fine.
 
minits said:
Summary:: Covariant derivative of the Riemann tensor evaluated in Riemann normal coordinates

Hello everyone,

in equation 3.86 of this online version of Carroll´s lecture notes on general relativity (https://ned.ipac.caltech.edu/level5/March01/Carroll3/Carroll3.html) the covariant derviative of the Riemann tensor is simply given by the partial derivative, the terms carrying the Christoffel symbols seem to vanish. I assume this results from the note that it is evaluated in Riemann normal coordinates. I know one can choose the coordinate system so that a given Christoffel-symbol vanishes but in this case there are so many to handle so that I am not convinced this is working. Can someone please give me an input on how to make myself clear that it works? Thanks in advance!
Riemann normal coordinates are, by definition, coordinates in which at a specific point ##x_0## the metric is minkowskian and (all) the Christoffel symbols vanish.
Therefore covariant derivatives evaluated at this point ##x_0## are just ordinary derivatives.
 
Thanks for your answer! I thought in this case the Riemann tensor should vanish as well due to it´s definition in form of products and derivatives of Christoffel symbols but one will probably simply use the argument that tensors are independent of any basis.
 
minits said:
I thought in this case the Riemann tensor should vanish as well due to it´s definition in form of products and derivatives of Christoffel symbols
The Christoffel symbols vanish at the origin of Riemann normal coordinates, but their derivatives do not vanish at that point. So the Riemann tensor, since it includes derivatives of the Christoffel symbols, does not vanish at that point.
 
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Ah ok thanks for your answer!
 

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