For our discussion, we'll assume that we're working with $\mathbb{R}^m$ only, but much or all of the following discussion should be carried over immediately to any finite dimensional inner product space.
For completeness, we'll state a few definitions, that'll be used in the questions that follow.
1) Tensors: We'll call $T$ a tensor of order $k$ (or just a $k$-tensor) on $\mathbb{R}^m$ if $T:(\mathbb{R}^m)^k\to \mathbb{R}$ is a $k$-linear map.
2) Tensor product of two $1$-linear forms on $\mathbb{R}^m:$
Let $A, B: \mathbb{R}^m\to \mathbb{R}$ be two $1$-linear forms. Then we define their tensor product $A\otimes B$ to be the bilinear form: $A\otimes B: (v,w)\mapsto A(v)B(w).$
3) Constructing a $k$-tensor from just one vector: Identifying $\mathbb{R}^m$ with its dual thanks to the canonical inner product on $\mathbb{R}^m,$ we can think of any vector $v$ as a $1$-linear form, and $v\otimes v\otimes \dots \otimes v =:v^{\otimes k}$ as a $k$-linear form (i.e. a $k$-tensor).
4) Symmetry: We define $T$ to be symmetric if $T(\sigma(v_1),\dots \sigma(v_n))=T(v_1\dots v_n)$ for every permutation $\sigma.$
5) Diagonalizability and orthogonal diagonalizability : Let $\{v_1\dots v_m\}$ be a basis for $\mathbb{R}^m.$ We say that $T$ is diagonalizable if there exist $\lambda_i\in \mathbb{R}, 1\le i \le m,$ so that $T=\sum_{i=1}^{k}\lambda_iv_i^{\otimes k}.$ Furthermore, we define $T$ to be orthogonally diagonalizable (in short, odeco, following this paper) if $v_i's$ form an orthonormal basis for $\mathbb{R}^m.$ Note that $T$ is odeco implies that there exists $R\in O(n), R:=[v_1\dots v_m],$ so that $T(x\dots x)=\sum_{i=1}^{m}\lambda_i(Rx)_i^k.$
P.S. The paper linked above, as well this paper do not define diagonalizability of a tensor, although they do orthogonally diagonalizable. I made up the former definition just by dropping the assumption that the basis need not be orthonormal. Also they used the word "orthogonally decomposable" instead of "orthogonally diagonalizable."
Here are my questions:
- By the definition above, all diagonalizable tensors are symmetric (but this is not the case for matrices, so I'm having trouble here - did I define diagonalizability of a tensor correctly?)
- When $k=2,$ a tensor becomes a bilinear form, that correspond to a matrix after choosing a basis. We know, thanks to the spectral theorem, that symmetry of a matrix is equivalent to orthogonal diagonalizability. However, the papers linked above claim that there that this is not so for higher order tensors. What's an example of a symmetric tensor that is not orthogonally diagonalizable (with proof), please?
- Density(?): What's an appropriate topology (ideally a metrizable one) on the space of $k$-tensors, and in this topology, can we approximate a symmetric tensor by a sequence of orthogonally diagonalizable tensors? If no, then how about a sequence of diagonalizable tensors?
Relevant references very highly appreciated! I'll take the liberty to add a few, as it appears that tensors have been of interest in the signal processing community more than the math community.