Is the Dual Basis in Minkowski Space Affected by the Metric Tensor?

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SUMMARY

The discussion centers on the relationship between the dual basis and the metric tensor in Minkowski space. It establishes that while an orthonormal basis typically allows for straightforward application of the metric tensor to derive the dual basis, Minkowski space introduces complexities due to the possibility of a dot product yielding -1. Despite this, the definition of the dual basis remains consistent across different metrics, as demonstrated with the coordinate basis vectors {∂t, ∂x, ∂y, ∂z} and their corresponding dual basis {dt, dx, dy, dz}, which adhere to the metric-independent relation ∂µ⋅dxγ = δµγ.

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  • Understanding of Minkowski space and its properties
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  • Basic grasp of differential forms and their applications
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This discussion is beneficial for theoretical physicists, mathematicians specializing in geometry, and students studying general relativity or differential geometry.

NanakiXIII
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Normally, if you have an orthonormal basis for a space, you can just apply your metric tensor to get your dual basis, since for an orthonormal basis all the dot products between the base vectors will boil down to a Kronecker delta. However, in Minkowski space, the dot product between a unit vector and itself may also be -1, rather than just 1, so a base vector like this does not meet the requirements if you're constructing your dual basis. Does that mean that simply applying your metric tensor need not produce your dual basis? Or does the definition of the dual basis change to allow the -1?
 
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The definition of the dual basis is the same in any space (doesn't matter what the metric is). If you take the coordinate basis vectors {∂t, ∂x, ∂y, ∂z} as the basis for the tangent space, then the dual basis is {dt, dx, dy, dz}, which satisfy

µ⋅dxγ = δµγ

Notice that these are metric independent relations. The action of a 1-form on a vector is independent of metric.
 
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Alright, that clears it up, thanks.
 

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