A lower-bound conjecture for the tripartite nullity

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Let V1,V2,V3V_1,V_2,V_3 be the local qudit vector spaces with dimensions d1,d2,d3d_1,d_2,d_3, and let nan_a be the corresponding one-party nullities. For a tripartite state v∈V1⊗V2⊗V3v\in V_1\otimes V_2\otimes V_3, let n1,2,3n_{1,2,3} denote the nullity of the common kernel space K1,2,3(v)K_{1,2,3}(v). The tripartite-nullity lower-bound conjecture. The nullity n1,2,3n_{1,2,3} satisfies

n1,2,3≥max⁡{(d1d2−d3+n3)n3,(d1d3−d2+n2)n2,(d2d3−d1+n1)n1}.n_{1,2,3}\ge\max\bigl\{(d_{1}d_{2}-d_{3}+n_{3})n_{3},(d_{1}d_{3}-d_{2}+n_{2})n_{2},(d_{2}d_{3}-d_{1}+n_{1})n_{1}\bigr\}.

The authors report extensive empirical evidence for this lower bound, which is intended to improve the available estimates for the invariant controlling tripartite entanglement classes; 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

Refreshed
Claimed solved

A reader-posted argument claims a complete proof of the conjecture, but it has not been independently checked, so the result is not settled.

Buniy and Kephart proposed the conjecture in December 2024: the common-kernel nullity should exceed an explicit maximum determined by the dimensions and one-party nullities.

Known results

The authors report extensive empirical evidence, but state that they have only upper and lower bounds for n1,2,3n_{1,2,3} and no complete result.

Posted attempt

A reader claims a complete proof by showing, for each permutation (i,j,k)(i,j,k), that Ki(v)⊗ker⁡fj,k(v)⊆K1,2,3(v)K_i(v)\otimes\ker f_{j,k}(v)\subseteq K_{1,2,3}(v); dimension counting then gives each term in the conjectured maximum. The argument has not been independently verified.

Current status (as of August 2026): The conjecture has a complete-proof claim based on an unverified reader argument; no independently corroborated proof or counterexample is recorded.

Sources

Solutions 1

ProofThis solution needs a summarySee full solutionHide full solution

Let v∈V1⊗V2⊗V3v\in V_1\otimes V_2\otimes V_3, put di=dim⁡Vid_i=\dim V_i, ni=dim⁡Ki(v)n_i=\dim K_i(v), and set ri=di−nir_i=d_i-n_i. Thus rir_i is the rank of the ii-th flattening of vv.

For each permutation (i,j,k)(i,j,k) of (1,2,3)(1,2,3), the two-party contraction

fj,k(v):Vj⊗Vk⟶Vi∗f_{j,k}(v):V_j\otimes V_k\longrightarrow V_i^*

has rank rir_i, and hence

dim⁡ker⁡fj,k(v)=djdk−ri.\dim\ker f_{j,k}(v)=d_jd_k-r_i.

For u∈Ki(v)u\in K_i(v) and z∈ker⁡fj,k(v)z\in\ker f_{j,k}(v), the tensor u⊗zu\otimes z belongs to the common kernel K1,2,3(v)K_{1,2,3}(v). Indeed, the (j,k)(j,k)-contraction vanishes because z∈ker⁡fj,k(v)z\in\ker f_{j,k}(v), and each of the other two pair contractions vanishes because u∈Ki(v)u\in K_i(v). Consequently,

Ki(v)⊗ker⁡fj,k(v)⊆K1,2,3(v),K_i(v)\otimes\ker f_{j,k}(v)\subseteq K_{1,2,3}(v),

so

n1,2,3(v)≥ni(djdk−ri)=ni(djdk−di+ni).n_{1,2,3}(v)\geq n_i(d_jd_k-r_i) =n_i(d_jd_k-d_i+n_i).

Taking the maximum over i=1,2,3i=1,2,3 gives precisely the asserted lower bound for every tripartite tensor, including the zero tensor.