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A generalization of Kruskal's theorem on tensor decomposition


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Benjamin Lovitz, Fedor Petrov, "A generalization of Kruskal's theorem on tensor decomposition," Forum of Mathematics, Sigma 11 (2023), e27, doi:10.1017/fms.2023.20 (arXiv:2103.15633v2, 2021).

Summary

The paper studies finite multisets of product tensors E={xa=xa,1⊗⋯⊗xa,m:a∈[n]}E=\{x_a=x_{a,1}\otimes\cdots\otimes x_{a,m}:a\in[n]\} over an arbitrary field. Its central result is the splitting theorem, Theorem 4: if dj=dim⁡span⁡{xa,j:a∈[n]}d_j=\dim\operatorname{span}\{x_{a,j}:a\in[n]\} and dim⁡span⁡(E)≤∑j(dj−1)\dim\operatorname{span}(E)\leq\sum_j(d_j-1), then EE splits as a direct sum of two nonempty subfamilies, or equivalently is disconnected as a matroid in the sense of Definition 3. Section 4 proves this by reducing to the two-factor estimate in Theorem 6, using preservation of connectedness under passage to factors (Proposition 5) and an ear decomposition of a connected matroid (Lemma 7). Fact 13 and Section 6 show that the numerical threshold is sharp, including for symmetric product tensors in the indicated characteristic-zero construction.

Corollary 10 replaces dim⁡span⁡(E)\dim\operatorname{span}(E) by the cardinality bound n≤∑j(dj−1)+1n\leq\sum_j(d_j-1)+1. This is the engine behind Theorem 2, the paper's generalization of Kruskal's theorem: if, for every S⊆[n]S\subseteq[n] with 2≤∣S∣≤n2\leq |S|\leq n,

2∣S∣≤∑j=1m(djS−1)+1,djS=dim⁡span⁡{xa,j:a∈S},2|S|\leq\sum_{j=1}^m(d_j^S-1)+1, \qquad d_j^S=\dim\operatorname{span}\{x_{a,j}:a\in S\},

then ∑axa\sum_a x_a is a unique tensor-rank decomposition. The proof adjoins the negatives of the terms in a competing decomposition and analyzes the connected components of the resulting zero-sum family. Unlike Theorem 1, which uses global Kruskal ranks, Theorem 2 uses ordinary ranks on all subfamilies and can apply below the Kruskal-rank threshold. Theorem 11 gives a reshaped form in which the partition of the tensor factors may vary with SS; Section 10 compares the three-factor criterion with the conditions of Domanov, De Lathauwer, and Sørensen, synthesizes those earlier criteria in Theorem 36, and ends with Question 38 on whether Condition U alone implies uniqueness.

Sections 7--9 develop further consequences of splitting. Theorem 15 and Corollaries 16--21 interpolate between linear independence, control of low-rank tensors in the span, and uniqueness, while Theorems 22 and 27 give partial coincidence results for decompositions having more terms than a known decomposition. In particular, Corollary 21 says that a circuit of product tensors can have dj>1d_j>1 in at most n−2n-2 factors. Theorem 28 gives a tensor-rank lower bound in terms of the standard ranks djd_j, Kruskal ranks kjk_j, and μ=max⁡i≠j(di−ki+dj−kj)\mu=\max_{i\ne j}(d_i-k_i+d_j-k_j), under the balance conditions ki≤∑j≠i(kj−1)+1k_i\leq\sum_{j\ne i}(k_j-1)+1; for two factors it specializes to Sylvester's matrix-rank inequality. Corollary 31 is the corresponding Waring-rank bound. For symmetric decompositions over fields of characteristic zero or characteristic greater than the tensor order, Theorem 32 shows that two distinct decompositions satisfying the stated Kruskal-rank hypotheses must have total number of terms n+r≥m+2d−2n+r\geq m+2d-2; Corollary 33 converts this to uniqueness even among certain nonminimal symmetric decompositions. Sections 8.1 and 9.1 provide broad sharpness constructions for these bounds.

Relation to E0774

For a finite set A⊂ZA\subset\mathbb Z, dissociation means that there is no nonzero relation ∑a∈Aεaa=0\sum_{a\in A}\varepsilon_a a=0 with εa∈{−1,0,1}\varepsilon_a\in\{-1,0,1\}. Thus the inclusion-minimal supports of such relations form a hypergraph on AA: dissociated subsets are precisely its independent sets, and a partition into finitely many dissociated sets is a finite proper coloring of this relation hypergraph. Proportionate dissociation gives a uniform positive lower bound on the independence ratio of every finite induced subhypergraph; E0774 asks whether the special hypergraphs arising from integer relations must consequently have bounded chromatic number.