Can one diagonalize the Kerr metric?

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SUMMARY

The discussion centers on the diagonalization of the Kerr metric in Boyer-Lindquist coordinates. It is established that while every spacetime metric is diagonalizable, this does not guarantee the existence of a coordinate system that achieves this for the Kerr metric, particularly due to its non-static nature. The theorem by Achille Papapetrou is referenced, indicating that the metric must be well-behaved on the axis of rotation for diagonalization to be feasible. The participants conclude that diagonalization may not be possible everywhere, especially on the axis of rotation.

PREREQUISITES
  • Understanding of Kerr metric and its properties
  • Familiarity with Boyer-Lindquist coordinates
  • Knowledge of diagonalization in the context of matrices
  • Basic principles of general relativity and spacetime metrics
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  • Research the implications of Achille Papapetrou's theorem on metric diagonalization
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  • Explore alternative coordinate systems for the Kerr metric
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The discussion is beneficial for physicists, mathematicians, and students specializing in general relativity, particularly those interested in the properties of the Kerr metric and its implications in theoretical physics.

arroy_0205
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Is it possible to diagonalize the Kerr metric in the Boyer-Lindquist coordinates? If so then I think calculations with the metric will become easier. I forget under what condition a matrix can be diagonalized. Can anybody remind me?
 
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I think if you transform to a co-rotating frame, the off-diagonal term will be zero. I might try it when I have more time.

[edit] I have since discovered that this transformation does not diagonalise the metric.

M
 
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Unfortunately, it is not possible. The reason that one can get as close as one off-diagonal term is a theorem by Achille Papapetrou. This requires that the metric be well-behaved on the axis of rotation. (Roy Kerr)
 
Sorry to bump an old thread, but is it possible to diagonalize the metric every where except on the axis of rotation? In other words, is the problem that no general diagonalization exists, or that it is simply a non-diagonalizable matrix? The second seems improbable to me, since the metric is symmetric and thus always diagonalizable, even unitarily, but I don't know much about the Kerr solution so maybe something weird is going on.
 
Notice who made post #3.

Every spacetime metric is diagonalizable, but not necessarily by a coordinate basis, i.e., there does not necessarily exist a coordinate system that diagonalizes the metric.
 
Isn't diagonalizability in a certain choice of coordinates equivalent to staticity? Since the Kerr metric isn't static, it seems to me that we don't need no fancy theorems as claimed in #3. Am I oversimplifying or getting something wrong?
 

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