Complex Metric Tensor: Meaning, Weak Gravitational Fields & Einstein Eqns

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SUMMARY

The discussion centers on the implications of a complex metric tensor, hαβ, within the context of linearized Einstein field equations in weak gravitational fields. Participants clarify that while tensors are not numbers, the components of the metric tensor must be real if the coordinate system employs real numbers. The consensus is that if the perturbation components, hmn, are complex, one can take the real part for practical purposes. Additionally, the use of complex exponentials in solutions may lead to confusion regarding the nature of the metric tensor.

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  • Familiarity with tensor mathematics and properties
  • Knowledge of symmetric matrices and eigenvalues
  • Basic concepts of wave equations in physics
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Physicists, mathematicians, and students studying general relativity, particularly those interested in the mathematical foundations of gravitational theories and the behavior of metric tensors in weak fields.

ngkamsengpeter
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I am working on the weak gravitational field by using linearized einstein field equation. What if the metric tensor, hαβ turn out to be a complex numbers? What is the physical meaning of the complex metric tensor? Can I just take it's real part?

Or there is no such thing as complex metric tensor and my system is not physically make sense?
 
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I really don't know what you mean by a metric tensor turning out to be a "complex number". A tensor is NOT number to begin with. And if your coordinate system uses real numbers to as coordinates then the components of the tensor must be real numbers. Of course, in a given coordinate system, we can think of a tensor as represented by a matrix and so find its eigenvalues. It is possible for the eigenvalues of a general matrix to be complex but the metric tensor should always be represented by a symmetric matrix which must have real eigenvalues.
 
Since you're working with the linearized field equations, on a Minkowski background presumably, yes you can just take the real part.
 
HallsofIvy said:
I really don't know what you mean by a metric tensor turning out to be a "complex number". A tensor is NOT number to begin with. And if your coordinate system uses real numbers to as coordinates then the components of the tensor must be real numbers. Of course, in a given coordinate system, we can think of a tensor as represented by a matrix and so find its eigenvalues. It is possible for the eigenvalues of a general matrix to be complex but the metric tensor should always be represented by a symmetric matrix which must have real eigenvalues.

What I mean here is that the component of the hmn turn out to be a complex numbers. That is h11 is a complex numbers. In linearized einstein field equation, metric tensor is just sum of flat spacetime metric plus the small pertubation hmn. So if component of hmn is a complex number, so I would think that the metric tensor is also complex. Or should I just take the real part as what Bill_K said?

Thanks.
 
Are you using dx0=ct or dx0=ict? This could be part of the difficulty.

Chet
 
Solving the linearized field equations amounts to solving the wave equation, so if your solution turns out to be complex there must be a fairly simple reason for it. Like you used exp(ikx-iwt) instead of sin and cos.
 
You have to give more details on how you arrived at a comples metric.
 

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