Undergrad Basic question, harmonic coordinate condition algebra

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SUMMARY

The discussion centers on the harmonic coordinate condition in general relativity, specifically addressing the covariant D'Alembertian operator ##\Box = \nabla^{\mu}\nabla_{\mu}## and its application in the context of the equation ##\Box x^{\mu} = 0##. Participants clarify the distinction between functions and vector components, emphasizing that the four functions ##x^{\mu}## are treated as functions rather than components. Key points include the vanishing of the double derivative in the first term and the proper handling of indices, particularly the correction of an error where ##\lambda## should be replaced with ##\mu## in the equations discussed.

PREREQUISITES
  • Understanding of covariant derivatives in differential geometry
  • Familiarity with the metric tensor and its properties
  • Knowledge of tensor notation and index manipulation
  • Basic concepts of general relativity and the role of harmonic coordinates
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  • Study the properties of the covariant D'Alembertian operator in general relativity
  • Learn about the implications of harmonic coordinates on the Einstein field equations
  • Explore the derivation and applications of equation 4.85 from Sean Carroll's lecture notes
  • Investigate the significance of the Kronecker delta in tensor calculus
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This discussion is beneficial for students and researchers in theoretical physics, particularly those focusing on general relativity, differential geometry, and tensor analysis. It is especially relevant for anyone looking to deepen their understanding of harmonic coordinates and their mathematical foundations.

binbagsss
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where ##□=\nabla^{\mu}\nabla_{\mu}## is the covariant D'Alembertian.

##□x^{\mu}=0##

##g^{\rho\sigma}\partial_{\rho}\partial_{\sigma}x^{\mu}-g^{\rho\sigma}T^{\lambda}_{\rho\sigma}\partial_{\lambda}x^{\mu}=0##

So this line is fine by subbing in the covariant derivative definition and lowering index using the metric.

The notes say that it is crucial to realize that when we take the covariant derivative that the four functions ##x^{\mu}## are just functions, not component of a vector. And I guess this is what he is using when he gets:

##g^{\rho\sigma}\partial_{\rho}\partial_{\sigma}x^{\mu}-g^{\rho\sigma}T^{\lambda}_{\rho\sigma}\partial_{\lambda}x^{\mu}=-g^{\rho\sigma}T^{\lambda}_{\rho\sigma}## ,
where ##T^{\lambda}_{\rho\sigma}## is the connection.

Excuse my stupid questions to follow, but I have no idea what is going on here:
- why has the double derivative of the first term vanished whilst a single derivative of the second does not?
- how has , I think he must have used that## \partial_{\lambda}x^{\mu}=1##, where has this came from?

All I can think of is some conditions imposed on the functions such as each four function is made to depend only upon one of ##x^\mu## and normalization.

Thanks in advance.

(Sean Carroll Lecture notes on GR, equation 4.85)
 
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binbagsss said:
why has the double derivative of the first term vanished whilst a single derivative of the second does not?
What is ##\partial_\nu x^\mu##?

Your equation is also wrong, the right side has ##\lambda## as a free index while the left does not.
 
Orodruin said:
What is ##\partial_\nu x^\mu##?

Your equation is also wrong, the right side has ##\lambda## as a free index while the left does not.

Equation 4.85, http://arxiv.org/pdf/gr-qc/9712019.pdf, that's what I thought.

##\partial_\nu=\frac{\partial}{\partial x^{\nu}}##
 
binbagsss said:
Equation 4.85, http://arxiv.org/pdf/gr-qc/9712019.pdf, that's what I thought.

##\partial_\nu=\frac{\partial}{\partial x^{\nu}}##
Obvious typo, also the fix is obvious (the ##\lambda## in the last expression should be a ##\mu##).

So what is ##\partial x^\mu/\partial x^\nu##?
 
Orodruin said:
Obvious typo, also the fix is obvious (the ##\lambda## in the last expression should be a ##\mu##).

So what is ##\partial x^\mu/\partial x^\nu##?

I thought he may have renamed ##\lambda## and ##\mu##. The fix wasn't so obvious for me, but ta...

##\partial x^\mu/\partial x^\nu=\delta^\mu_\nu##?
 
binbagsss said:
##\partial x^\mu/\partial x^\nu=\delta^\mu_\nu##?

Right, so is it clear how equation (4.85) follows?
 
Orodruin said:
Right, so is it clear how equation (4.85) follows?

ahhh ofc, thanks.
 

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