Prove Levi-Civita Symbol is Only 3D Isotropic Tensor

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Discussion Overview

The discussion revolves around the properties of the Levi-Civita symbol as an isotropic tensor in three-dimensional space, exploring its uniqueness and the implications of isotropy under the group of spatial rotations, SO(3). Participants examine the mathematical foundations and seek proofs related to this concept.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant notes that their fluid mechanics textbook claims the Levi-Civita symbol is isotropic but does not provide a proof, prompting questions about its uniqueness as the only isotropic tensor in 3D space.
  • Another participant clarifies that isotropic means invariant under rotations from SO(3) and suggests deriving invariant tensors through group decomposition, mentioning the tensor product of vectors and its relation to the Levi-Civita tensor.
  • A participant emphasizes that a completely antisymmetric 3-tensor in 3D has one independent component, which leads to the conclusion that it is effectively a scalar, thus supporting the isotropy of the Levi-Civita tensor.
  • One participant expresses interest in finding a detailed proof of the claims made, indicating they are currently studying group representation theory.
  • Another participant suggests a text by Georgi on Lie groups as a potential resource for further reading.
  • A different participant mentions finding an elementary proof in a book by Rutherford Aris, outlining a method to show the Levi-Civita's invariance and its necessity for a rank-3 tensor to be isotropic.
  • One participant raises a question about the terminology "tensor density," seeking clarification on its relation to density.

Areas of Agreement / Disagreement

Participants generally agree on the isotropic nature of the Levi-Civita symbol under SO(3) but do not reach a consensus on the uniqueness of the Levi-Civita tensor as the only isotropic tensor in 3D space. The discussion includes multiple perspectives on proofs and methods of understanding the concept.

Contextual Notes

Some limitations include the dependence on specific definitions of isotropy and the group SO(3), as well as the unresolved nature of the uniqueness claim regarding isotropic tensors in three dimensions.

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My fluid mechanics textbook says so but gives no proof, I see why it's isotropic but I can't think of why it's the only isotropic tensor in 3D space.
 
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What does isotropic here mean? Invariant under rotations (elements from SO(3) )?

I have the feeling you should be a bit more precise. Usually, one derives invariant tensors under specific group elements from group decomposition. You're working in three dimensional Euclidean space, so you should look at spatial rotations, which are elements of SO(3). For instance, if you denote by V the vector representation of SO(3) and by S the scalar representation, one should have

<br /> V \otimes V \otimes V = S_A + \ldots<br />

This means that the tensor product of three vectors can be decomposed in a completely antisymmetric part (which is the meaning of the subscript A) plus other stuff not important for your question. A completely antisymmetric 3-tensor in 3 dimensions has one independent component (check this!), and hence is "effectively a scalar". This shows that one has an invariant (isotropic!) tensor in three dimensions which is completely antisymmetric: the Levi-Civita 'tensor'.

Note that this is not a tensor for general transformations; one uses the fact that the determinant of an element of SO(3) is +1. Technically, it is a tensor density!
 


thanks, I meant invariant under SO(3). Actually I'm learning some group representation theory now but haven't gone far, so I guess I'll save you post for reading in more details later. And where can I read a detailed proof on this?
 


thanks, I meant invariant under SO(3). Actually I'm learning some group representation theory now but haven't gone far, so I guess I'll save you post for reading in more details later. And where can I read a detailed proof on this?
 


Perhaps it's somewhere in Georgi's text on Lie groups :)
 


I found a elementary proof of this, I don't know if the group method is neater or not, but this one is definitely much more elementary. It's in a book called "Vectors, tensors, and the basic equations of fluid mechanics" by Rutherford Aris, and method can be found in chap 2.7. The basic idea is to first show Levi-Civita is indeed invariant, second by considering a few special rotations to show that if a rank-3 3-D tensor has to be Levi-Civita before it can be an isotropic tensor.
 


Actually I'm a bit curious of the nomenclature of "tensor density".It's obvious why it's called "relative tensor", but what does it have anything to do with density?
 

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