Let be unital associative algebras over a field, each a simple ring, and a two-sided ideal of their tensor product. Choose of minimal two-factor tensor rank. Both factor families are linearly independent. Since , choose and replace by . The result has first coefficient , is nonzero by the linear independence of the , and retains minimal two-factor tensor rank; its first factor family is therefore still linearly independent. Now apply the same construction in to make the first second-factor coefficient . The result is again nonzero of minimal two-factor tensor rank, and both its coefficient families are linearly independent.
If , commutation with gives a tensor in expressible with at most pure tensors, hence zero by minimality. Independence forces every to be central, hence a scalar multiple of . Independence of then forces . Thus , proving simplicity of the tensor product without a splitting-field argument.
Keep the nonzero of minimal two-factor tensor rank constructed in part (i). For every , its commutator with lies in and equals
If this tensor were nonzero, its two-factor tensor rank would be at most , contradicting minimality. Thus it is zero. The linear independence of forces for every and . Since , each is a scalar multiple of .
But are linearly independent. Hence , so . A two-sided ideal containing the multiplicative identity is the entire ring; therefore .
We have proved the stronger result that is a simple ring. It has finite dimension , so part (b) proves
Part (c)(ii) also gives , so this proves that a tensor product of central simple algebras is again a central simple algebra.
Let be a two-sided ideal of . Choose a nonzero of least possible two-factor tensor rank , and take a shortest expression
Both families and are linearly independent: a linear dependence in either family would combine terms and shorten the expression. In particular .
Because is a simple ring, the two-sided ideal generated by is . Thus there are finitely many with . Form
Since the are linearly independent, applying a linear functional selecting shows . Its two-factor tensor rank is at most and hence, by the choice of , exactly . Consequently are linearly independent.
Similarly, simplicity of gives finitely many with . Now
The linear independence of the shows , and minimality again makes its two-factor tensor rank exactly . We have obtained
Both coefficient families in this expression are linearly independent. Retaining this additional property is the key to the next part. This is coefficient normalization in an ideal of a tensor product.
Two-factor tensor rank 2026-10-14
The two-factor tensor rank is the smallest number of pure tensors whose sum equals , with zero allowed as the empty sum. For two finite-dimensional vector spaces over the same field, it equals the matrix rank of the tensor-product coefficient matrix. A sum of outer products has column space contained in the span of their first factors, so its matrix rank is at most . Conversely, choose a basis for the column space, express each column in that basis, and collect the coefficients into row vectors . This yields , hence a sum of pure tensors.
The pure tensor therefore has two-factor tensor rank one, whereas has two-factor tensor rank two. Both have two factors: the number of factors and the minimum number of product summands are different counts. Over the real numbers, the singular value decomposition supplies a useful decomposition , with one nonzero term per matrix rank. The two-factor rank equality does not extend to three or more factors by merely choosing one matrix layout.