An improved lower-bound conjecture for the tripartite nullity
An improved 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 improved tripartite-nullity lower-bound conjecture. The nullity satisfies
This is presented as a stronger empirically supported lower bound for the tripartite nullity and hence for the analysis of tripartite entanglement classes. Its validity remains open.
Progress summary
A 2024 paper left the stronger bound open, while a posted argument claims a complete proof that has not been independently verified.
Buniy and Kephart proposed the improved lower bound in 2024 for the common nullity of a tripartite tensor, strengthening earlier bounds. The paper records it as Conjecture 3.4 and leaves its validity unresolved.
Known results
- Buniy and Kephart (2024) report extensive empirical evidence for the lower-bound conjectures.
- The allowed values of the three one-party nullities are characterized completely, but only lower and upper bounds are known for .
Posted attempt
A reader-written argument claims a complete proof: after decomposing into active and null sectors, it derives an identity reducing the conjectured inequality to . This attempt has not been independently verified.
Current status (as of August 2026): The conjecture has empirical support and a posted unverified proof attempt, but no independently verified proof or counterexample is recorded.
Sources
Sources & referencesView supporting material
Primary source
Roman V. Buniy and Thomas W. Kephart, “Tripartite entanglement of qudits”, arXiv:2412.10728 (2024).
Solutions 1
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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
Therefore their maximum equals
Subtracting the proposed lower bound from (2) leaves exactly
Hence the conjectured inequality holds for every tripartite tensor.