A strengthened lower-bound conjecture for the tripartite nullity
Let be the local qudit vector spaces with dimensions , and let be the corresponding one-party nullities. For a tripartite state , let denote the nullity of the common kernel space . The strengthened tripartite-nullity lower-bound conjecture. The nullity satisfies
The additional minimum term strengthens the preceding empirical lower bound and is proposed as part of the authors' conjectural description of the tripartite nullity. Its general validity remains open.
References
Primary source
Roman V. Buniy and Thomas W. Kephart, “Tripartite entanglement of qudits”, arXiv:2412.10728 (2024).
Progress summary
A reader claims a complete proof of the strengthened conjecture, but no independent verification has been found.
The conjecture proposes an additional minimum term in the lower bound for the common kernel of a tripartite tensor. Buniy and Kephart introduced this conjectural bound in their 2024 study of tripartite qudit entanglement.
Posted attempt
A reader claims a complete proof by decomposing the tensor into active and null-coordinate sectors, obtaining an exact formula whose remaining term is a nonnegative common-kernel dimension. The argument has not been independently verified, so it establishes only a claimed resolution.
Current status (as of August 2026): A complete proof has been claimed in discussion, but the conjecture remains mathematically unsettled pending independent verification.
Sources
Solutions 1
ProofThis solution needs a summarySee full solution
Let , let , let , and set . Thus is the rank of the -th flattening of . Choose a basis in each factor and its corresponding dual basis so that is supported on
with complementary null-coordinate spaces of dimensions . Let be the common-kernel dimension of the three pair-contraction maps restricted to the active spaces.
Splitting the tensor in the common-kernel equations according to the eight coordinate sectors of
gives the exact identity
Indeed, the all-active sector contributes . In the sector , the contractions involving the first factor vanish automatically, while the remaining contraction has rank on , independently for each of the null coordinates. This sector therefore contributes ; the other one-null sectors follow by symmetry. Every sector containing at least two null factors is annihilated by all three pair contractions, giving the four remaining terms. Different support sectors have disjoint active/null output blocks, so these contributions form a direct sum.
Set
Then (1) becomes
The three expressions inside the maximum in the conjectured bound are respectively
and those inside its minimum are . Thus
Consequently the entire conjectured lower bound is exactly . Formula (2) shows that the actual tripartite nullity exceeds this bound by precisely . Therefore the strengthened conjecture holds for every tripartite tensor, and (1) gives the exact additional nonnegative term.