Sign conventions in general relativity

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SUMMARY

This discussion focuses on the complexities of sign conventions in general relativity, particularly regarding the definitions of the Riemann tensor, Ricci tensor, and the stress-energy tensor. Participants highlight the variations in sign conventions across different texts, notably Misner, Thorne, and Wheeler, and emphasize the impact these conventions have on the Einstein field equations. A specific resource, a scanned chart from Misner, is referenced as a helpful summary of these conventions. The conversation also touches on the independence of Christoffel symbols from the sign of the metric tensor.

PREREQUISITES
  • Understanding of Riemann and Ricci tensors in general relativity
  • Familiarity with Einstein field equations and their formulations
  • Knowledge of Christoffel symbols and their role in tensor calculus
  • Access to key texts such as Misner, Thorne, and Wheeler's "Gravitation"
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  • Research the differences in sign conventions in general relativity literature
  • Study the derivation of the Riemann tensor and its implications on the Ricci tensor
  • Examine the role of Christoffel symbols in tensor definitions and calculations
  • Explore the MAXIMA software for practical applications of Ricci tensor calculations
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Physicists, mathematicians, and students of general relativity seeking clarity on sign conventions and their implications in tensor calculus and Einstein's equations.

Nabigh R
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Hi guys... I was wondering if anyone have a sort of a summary of sign conventions in general relativity books. By convention I mean the definition of Riemann tensor, Ricci tensor and signs of stress-energy tensor and signs of einstein field equations for a given sign of metric tensor... I heard that there is a table that shows something like that in Misner, Thorne, Wheeler... can somebody please upload it as I don't have access to that book.

Thanks.
 
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Thanks ultrafast... I have already seen those and in fact it's because of the latter link only I posted this question... it's really hard to keep track of changes to the field equations with different conventions... I mean in one, the constant on right hand side is negative, other positive, even the form of stress-energy tensor of perfect fluid say, depends on sign convention and so forth. So I was wondering if anyone have a summary of how everything looks like with different conventions.
 
Someone had scanned in this famous chart:

http://itp.epfl.ch/webdav/site/itp/users/166340/public/Misner%28SignConvention%29.pdf

which is the origin of part of that wikipedia entry.
 
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Thanks a lot robphy. That really helps.
 
As an aside to the original question: the Christoffel symbols doesn't depend on the sign of metric, right?
What about other tensors found using them?
 
Nabigh R said:
As an aside to the original question: the Christoffel symbols doesn't depend on the sign of metric, right?
What about other tensors found using them?

For example, the Riemann tensor is defined in terms of them, but is anti-symmetric in its last two indeces and as such defining the Ricci-tensor in terms of contraction over the 1st and 3rd Vs 1st and 4th indeces yields a conventional sign difference relating the Einstein tensor to the stress-energy tensor. This is why you sometimes see a minus sign in front of the stress-energy tensor side even though its usually a plus.
 
waitedavid137 said:
For example, the Riemann tensor is defined in terms of them, but is anti-symmetric in its last two indeces and as such defining the Ricci-tensor in terms of contraction over the 1st and 3rd Vs 1st and 4th indeces yields a conventional sign difference relating the Einstein tensor to the stress-energy tensor. This is why you sometimes see a minus sign in front of the stress-energy tensor side even though its usually a plus.

Yeah David, I think even MAXIMA defines Ricci tensor in terms of contraction over 1st and 4th indices since it defines the Riemann tensor as in Weinberg (1972), but the components of Ricci tensor have opposite signs to the ones given by Weinberg.
 

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