Discreteness of asymptotic tensor ranks
Tensor parameters that are amortized or regularized over large tensor powers, often called "asymptotic" tensor parameters, play a central role in several areas including algebraic complexity theory (constructing fast matrix multiplication algorithms), quantum information (entanglement cost...
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Zusammenfassung: | Tensor parameters that are amortized or regularized over large tensor powers,
often called "asymptotic" tensor parameters, play a central role in several
areas including algebraic complexity theory (constructing fast matrix
multiplication algorithms), quantum information (entanglement cost and
distillable entanglement), and additive combinatorics (bounds on cap sets,
sunflower-free sets, etc.). Examples are the asymptotic tensor rank, asymptotic
slice rank and asymptotic subrank. Recent works (Costa-Dalai,
Blatter-Draisma-Rupniewski, Christandl-Gesmundo-Zuiddam) have investigated
notions of discreteness (no accumulation points) or "gaps" in the values of
such tensor parameters.
We prove a general discreteness theorem for asymptotic tensor parameters of
order-three tensors and use this to prove that (1) over any finite field (and
in fact any finite set of coefficients in any field), the asymptotic subrank
and the asymptotic slice rank have no accumulation points, and (2) over the
complex numbers, the asymptotic slice rank has no accumulation points.
Central to our approach are two new general lower bounds on the asymptotic
subrank of tensors, which measures how much a tensor can be diagonalized. The
first lower bound says that the asymptotic subrank of any concise three-tensor
is at least the cube-root of the smallest dimension. The second lower bound
says that any concise three-tensor that is "narrow enough" (has one dimension
much smaller than the other two) has maximal asymptotic subrank.
Our proofs rely on new lower bounds on the maximum rank in matrix subspaces
that are obtained by slicing a three-tensor in the three different directions.
We prove that for any concise tensor, the product of any two such maximum ranks
must be large, and as a consequence there are always two distinct directions
with large max-rank. |
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DOI: | 10.48550/arxiv.2306.01718 |