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RESEARCH / Focused target

The reduced function of the partial negativity is not concave

Literature status: not recheckedRepository record: refuted

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Problem

The question

Y. Guo, Partial-Norm of Entanglement: Entanglement Monotones That are not Monogamous, New J. Phys. 25 (2023) 083047, arXiv:2212.06521v6, states:

We conjecture that $\hat{h}$ is concave [Suppl].

For decreasing Schmidt coefficients $\lambda_1\ge\lambda_2\ge\cdots$, the paper defines $\hat N(|\psi\rangle)=\lambda_1\lambda_2$ and the reduced function $\hat h(\rho)=\sqrt{\delta_1\delta_2}$, where $\delta_j=\lambda_j^2$. Its definition of concavity is

$$ h(t\rho+(1-t)\sigma)\ge t h(\rho)+(1-t)h(\sigma),\qquad 0\le t\le1. $$

Issue #14495 preregisters the reading over every finite dimension $d\ge2$ and all positive semidefinite complex $d\times d$ matrices of trace one. The later paper Complete Genuine Multipartite Entanglement Monotone, arXiv:2301.00334v3, explicitly identifies $\delta_1,\delta_2$ as the two largest eigenvalues of $\rho$ and repeats the conjecture in its table footnote. Eigenvalues are counted with multiplicity; their positions are chosen separately for each state, rather than tied to fixed eigenvectors.

Motivation

Our foothold

The source's Proposition 1 states that an entanglement monotone's reduced function is concave. The partial-negativity section assumes monotonicity before deriving further statements. A failure of concavity therefore removes a premise used for that interpretation in general dimension. It does not, by itself, settle every separate statement about partial negativity, its convex-roof extension, or monogamy.

Gap

Missing bridges

The primary TeX sources of arXiv:2212.06521v6 and arXiv:2301.00334v3 retain the conjecture. The former's phrase "but it is not true for the higher dimensional case" concerns strict concavity: its displayed pair attains equality at the midpoint. It does not supply a violation of concavity. Reference [Suppl] additionally asserts the midpoint inequality for commuting states; the counterexample below has commuting diagonal states.

The arXiv metadata queries all:"partial negativity" AND all:concave and all:"partial-norm" AND all:entanglement each return only 2212.06521v6. Repository and pinned Mathlib searches do not identify a theorem settling this conjecture. These are bounded search results, not worldwide priority or absence claims. The standalone erratum with DOI 10.1016/j.rinp.2025.108408 remains unread; the read v3 of the later paper still contains the conjecture. The later paper asserts concavity in its prose, labels it a conjecture in the table, and explicitly assumes it later; those passages supply no proof of the conjecture.

Route

Proposed approach

Set $d=3$, $t=1/2$ and

$$ \rho=\operatorname{diag}(1/2,1/3,1/6),\qquad \sigma=\operatorname{diag}(1/2,1/6,1/3). $$

Both matrices are positive semidefinite and have trace one. Their characteristic polynomials are the products of their three diagonal linear factors. Their decreasing eigenvalue lists are both $(1/2,1/3,1/6)$, so $\hat h(\rho)=\hat h(\sigma)=\sqrt{1/6}$. Their midpoint is $\operatorname{diag}(1/2,1/4,1/4)$ and has reduced function $\sqrt{1/8}<\sqrt{1/6}$. This reverses the required inequality.

Falsifier

What would falsify this route

The meaning "two largest eigenvalues" is essential. Fixing the same two eigenvectors for both states changes the claim. The definition hhat uses the real parts of characteristic roots sorted in decreasing order. For Hermitian matrices these are the real eigenvalues with their multiplicities, as identified by Mathlib's Matrix.IsHermitian.sort_roots_charpoly_eq_eigenvalues₀. The default zero entries for lists shorter than two are irrelevant on the claim's domain $d\ge2$.

Evidence

Evidence to collect

The Lean source is D5/S3/Quantum/Entanglement/PartialNegativityConcavityRefutation.lean. Its sole public theorem result : ¬ claim is an unconditional negation of the universal density-matrix concavity claim. Its four private helper theorems identify the sorted diagonal spectrum, positivity, trace and mixture, and each occurs on the proof path of result. The definitions hhat and claim introduce no additional theorem or audit target. The direct import is Mathlib.Analysis.Matrix.Order; there is no project formal prerequisite, new axiom, sorry or native_decide.

The Blueprint describes the same definitions and negation. Statements about publications, physical realizability or other entanglement properties are source readings or manuscript arguments, not consequences certified by the Lean theorem.

Triage

Scope assessment

Tier 1 external named conjecture, preregistered in #14495. proof_shape: bind-only for result and all four consumed helpers; escape_witness: none; admission_basis: open-problem-resolution. The result's utility is certified-instance with basis refutes the closed definition claim. The designated literal result : ¬ claim is exempt from four-slot registration under CLAUDE.md §3.9; there are no other public theorems or lemmas in the module.

What the settlement shows

  • Proved by result: concavity fails in the universal finite-dimensional claim. The proof supplies positive semidefinite trace-one qutrit states and the legal mixing parameter $1/2$, so failure does not depend on a non-Hermitian extension or an inadmissible matrix.
  • Proved inside result for the displayed states: the two original sorted spectra give $\sqrt{1/6}$, while the midpoint gives $\sqrt{1/8}$. The second-largest value belongs to different basis vectors in the two states; mixing reduces it while preserving the largest value.
  • Manuscript argument, not a separate Lean theorem: the states commute, so commutativity alone cannot repair the conjecture or [Suppl]'s assertion. This observation does not characterize the state families on which concavity survives.
  • Source-attested, not formalized here: concavity for qubit states. The qutrit refutation does not contradict that restricted assertion.
  • Open here: a complete characterization of state families on which $\hat h$ is concave, including a proposed restriction to diagonal states with a common decreasing order, and the exact consequences for the source's monotonicity and monogamy results. The source's conditional results require their actual hypotheses; this refutation does not certify or refute their remaining arguments.

ASSUMED-UNVERIFIED

Unverified assumptions

The literature search is not exhaustive. The standalone Results in Physics erratum is not read: its publisher landing page supplies only a redirect and the Firecrawl proxy is unavailable without authentication. The full text of Monogamy of k-entanglement, Phys. Rev. A 110, 012405 (DOI 10.1103/PhysRevA.110.012405), is also unread: its PDF requires authorization and the same proxy is unavailable. The preregistration's other literature readings are attributed reports, not independent checks made by this source. No worldwide novelty, priority, physical preparation or measurement is certified. The kernel checks the mathematical encoding; correspondence to the published meaning is established by reading and independent fidelity review.

Dossier & anchor history

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