Calculating Covariant Derivative of Riemann Tensor in Riemann Normal Coordinates

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Discussion Overview

The discussion centers on the calculation of the covariant derivative of the Riemann tensor in Riemann normal coordinates, as presented in equation 3.86 of Carroll's lecture notes on general relativity. Participants explore the implications of using Riemann normal coordinates, particularly regarding the behavior of Christoffel symbols and the Riemann tensor itself.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about the application of Riemann normal coordinates, noting that while Christoffel symbols vanish at a point, there are many to consider, leading to uncertainty about the validity of the simplification in the covariant derivative.
  • Another participant asserts that in Riemann normal coordinates, covariant derivatives at a specific point reduce to ordinary derivatives due to the vanishing of all Christoffel symbols at that point.
  • A participant questions whether the Riemann tensor should also vanish at the origin of Riemann normal coordinates, referencing its definition involving products and derivatives of Christoffel symbols.
  • It is clarified that while Christoffel symbols vanish at the origin, their derivatives do not, implying that the Riemann tensor does not vanish at that point.

Areas of Agreement / Disagreement

Participants exhibit some agreement regarding the properties of Riemann normal coordinates, but there remains disagreement and uncertainty about the implications for the Riemann tensor and the validity of the simplifications made in the covariant derivative calculation.

Contextual Notes

Participants highlight the complexity of handling multiple Christoffel symbols and their derivatives, indicating that assumptions about their behavior in Riemann normal coordinates may not be straightforward.

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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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