components of antisymmetric tensor unchanged under rotations proof
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In "classical theory of fields" Landau states that the components of a completely antisymmetric tensor of a rank equal to the number of dimensions of the space remain unchanged after a rotation. I have not been able to prove it or find a proof. Is there an elegant way to show this?
tensors rotations special-relativity
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In "classical theory of fields" Landau states that the components of a completely antisymmetric tensor of a rank equal to the number of dimensions of the space remain unchanged after a rotation. I have not been able to prove it or find a proof. Is there an elegant way to show this?
tensors rotations special-relativity
add a comment |
up vote
0
down vote
favorite
up vote
0
down vote
favorite
In "classical theory of fields" Landau states that the components of a completely antisymmetric tensor of a rank equal to the number of dimensions of the space remain unchanged after a rotation. I have not been able to prove it or find a proof. Is there an elegant way to show this?
tensors rotations special-relativity
In "classical theory of fields" Landau states that the components of a completely antisymmetric tensor of a rank equal to the number of dimensions of the space remain unchanged after a rotation. I have not been able to prove it or find a proof. Is there an elegant way to show this?
tensors rotations special-relativity
tensors rotations special-relativity
asked Nov 16 at 21:49
wonszrzeczny
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