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Complete Existence Classification of Seven-Partite Absolutely Maximally Entangled States

T0 review · 0 major / 4 minor · reviewed 2026-08-06 · deepseek-v4-flash

Pith's one-line read Seven-qudit AME states exist exactly in local dimension $d\ge 3$.

desk verdict Settles the last open existence question for AME(7,d) with a genuinely new construction family; the proof is explicit and checkable, and the central argument holds up. read the letter →

arxiv 2608.01011 v1 pith:P3BLC5DF submitted 2026-08-02 quant-ph

classification quant-ph
keywords absolutelymaximallyentangledstatesAME(7d)sevenquditsquantumMDScodesquadratic-phaseSteanecodeFanoplaneHamming
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

This paper settles the existence problem for seven-partite absolutely maximally entangled states: an AME(7,d) state exists if and only if $d\ge 3$. The only negative case is $d=2$, already known, and the genuinely new work supplies explicit states in every odd dimension and every dimension congruent to 2 modulo 4. The odd-dimensional family is a cyclic quadratic-phase state built from the complement of the seven-cycle, and the twice-odd family couples the Steane-code logical basis to such phase states so that every three-party reduced density is maximally mixed. A reader should care because AME states are pure quantum MDS codes and are used in quantum secret sharing, parallel teleportation, and holographic error correction; closing the seven-party case removes an outstanding entry from the standard AME table.

What carries the argument

Two explicit state families carry the proof. The odd family is the cyclic quadratic-phase state $|G_q\rangle$ with phase matrix the upper-triangular part of the complement of the seven-cycle; the AME check becomes invertibility of $3\times3$ submatrices over $\mathbb{Z}_q$. The twice-odd family is the coupled state $|\Psi_{2q}\rangle=(|0_L\rangle|G_0^{(q)}\rangle+|1_L\rangle|G_1^{(q)}\rangle)/\sqrt{2}$, where $|0_L\rangle,|1_L\rangle$ are Steane-code logical states and $|G_a^{(q)}\rangle$ are one-qudit phase-shifted copies. The central mechanism is the complementary vanishing of the binary cross block (nonzero only on the seven Fano triples $L_t=\{t,t+1,t+3\}$) and the odd cross block (vanis

What would settle it

Build $|G_q\rangle$ from Eq. (4) for an odd composite, say $q=9$, using exact arithmetic, and compute each of the 35 three-party reduced density matrices $\rho_S=\operatorname{Tr}_{S^c}|G_q\rangle\langle G_q|$; the odd-dimensional branch is false if any $\rho_S\neq I/9^3$. A cheaper check is to compute the five representative determinants in Eq. (5) modulo $q$ and confirm, via translation invariance, that every one of the 35 regenerated $\Gamma_{S,R}$ has nonzero determinant modulo $q$.

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Extended reading notes

Core claim

The paper claims the complete classification AME(7,d) exists iff $d\ge 3$. For odd $q$, it constructs $|G_q\rangle=q^{-7/2}\sum_{x\in\mathbb{Z}_q^7}\omega_q^{Q(x)}|x\rangle$ with $Q(x)=x\tilde\Gamma x^T$ and $\Gamma$ the complement of the seven-cycle; by a cited criterion, checking the state is AME reduces to showing each of 35 three-by-three submatrices $\Gamma_{S,R}$ is invertible over $\mathbb{Z}_q$, which translation symmetry reduces to five determinant computations. For $d=2q$, it forms $|\Psi_{2q}\rangle=(|0_L\rangle|G_0^{(q)}\rangle+|1_L\rangle|G_1^{(q)}\rangle)/\sqrt{2}$, identifying the qubit-qudit basis with a qudit of dimension $2q$. The binary cross term $R_{01}^S$ vanishes on al

Load-bearing premise

The load-bearing premise is the cited Theorem 3 of Ref. [8] that a quadratic-phase state over $\mathbb{Z}_q^7$ is AME whenever, for every three-subset $S$, some $3\times3$ submatrix $\Gamma_{S,R}$ is invertible over $\mathbb{Z}_q$; the paper does not prove this theorem or restate its full hypotheses, so every odd-dimension state (and every composite dimension built from it) depends on it.

Editorial extensions

If this is right

  • For every $d\ge 3$, the paper gives explicit normalized pure states: Eq. (4) for odd $d$, Eq. (31) for $d\equiv2\pmod4$, and product or Reed-Solomon states for the remaining powers of two.
  • Every seven-partite system with local dimension $d\ge3$ admits a pure state maximally entangled across every bipartition, so the seven-party AME table is complete.
  • The previously open cases $\mathrm{AME}(7,6)$ and $\mathrm{AME}(7,10)$ are resolved, with explicit states written out in Eq. (40).
  • Since AME(7,d) is equivalent to a pure quantum MDS code $[[7,0,4]]_d$, the classification proves such codes exist exactly for $d\ge3$.
  • The failure at $d=2$ is isolated: no other local dimension obstructs seven-party absolutely maximally entangled states.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • One can view the construction as transferring the obstruction from the binary sector to a small exceptional set of cuts; this suggests a general recipe for AME$(n,2q)$ whenever the binary code has dual distance $\lfloor n/2\rfloor+1$ and the partner phase state kills the exceptional cuts.
  • The complete seven-party classification makes the qubit case $d=2$ look like the sole number-theoretic exception; it is natural to test the same binary-odd coupling on the next open case, AME(8,4).
  • Replacing $\mathbb{Z}_q$ in the phase state with other finite abelian groups, if the invertibility criterion carries over, would give a direct construction for even dimensions without invoking the product property, possibly simplifying the $\alpha\ge2$ branches.
  • Because AME(7,d) is a pure $[[7,0,4]]_d$ MDS code, the classification also closes the existence question for seven-qudit QMDS codes; the remaining hard cases shift to lengths $n\ge8$.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

0 major / 4 minor

Summary. The paper proves the complete existence classification of seven-partite absolutely maximally entangled states: AME(7,d) exists if and only if d ≥ 3. The proof is constructive. For every odd q ≥ 3, the cyclic quadratic-phase state |G_q> in Eq. (4) is shown to be AME by verifying, through the five translation representatives S = 012, 013, 014, 015, 024, that suitable 3×3 submatrices Γ_{S,R} have determinants −1, 1, 2, −1, 1, all units over Z_q for odd q. For d = 2q with q odd, the coupled state |Ψ_{2q}> in Eq. (31) combines the two logical states of the Steane code with the odd-dimensional states |G_0^{(q)}> and |G_1^{(q)}>. The binary cross-block R^S_{01} is shown to vanish on all 28 non-Fano three-subsets by a support argument using the simplex/Hamming code structure, and the odd-sector cross-block T^S_{01} is shown to vanish on the seven Fano cuts via the null-vector certificates in Table II. Together with the known nonexistence at d = 2, the known AME(7,4) state, the Reed–Solomon construction for powers of two, and the product property for AME states, the claimed classification follows.

Significance. If correct, this resolves previously open cases including AME(7,6) and AME(7,10), and completes the existence classification of AME states for all n ≤ 7. The constructions are explicit and checkable: the five submatrix determinants are computed, the Fano-cut cancellation is certified by the seven explicit null vectors in Table II, and Eq. (40) gives an explicit wavefunction for the twice-odd dimensions. The proof is largely self-contained, with only standard code-theoretic facts and one cited rank criterion used as inputs. The completeness of the case split in terms of d = 2^α m with m odd is clear. This is a clean and significant resolution of a well-known open problem.

minor comments (4)
  1. [Odd local dimensions, Eq. (6)] The proof of Eq. (6) relies entirely on Theorem 3 of Ref. [8], whose exact hypotheses are not restated. Since the classification requires composite odd dimensions (q = 9, 15, ...), please either quote the theorem's hypotheses explicitly or include the short character-orthogonality argument showing that the stated rank condition over Z_q is sufficient for every odd q. The argument is elementary, but as written the reader cannot verify the scope of the cited theorem.
  2. [Twice-odd local dimensions, Eq. (10)] The notation 'I23 23' in Eq. (10) is ambiguous; it should be written as I_{2^3}/2^3 (equivalently I_8/8).
  3. [Twice-odd local dimensions, before Eq. (34)] Typo: 'Accorrding' should be 'According'.
  4. [Twice-odd local dimensions, Eqs. (10) and (13)] The phrase 'the distance of C and (C+1) are both 4' could be misread, since C+1 contains words of weight 3. Please clarify that the minimum distance between distinct elements of the coset C+1 is 4 (as a nonlinear code), not the minimum Hamming weight of its elements.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity identified: constructions are explicit and the only self-citation is backed by an independent reference.

full rationale

The paper's central claim, AME(7,d) exists iff d≥3, is established by three independent construction families, each verified by direct computation rather than by assuming the conclusion. The odd-dimension branch uses Theorem 3 of Ref. [8] (Feng et al.), an external result that gives a sufficient condition for a quadratic-phase state to be AME; the paper then verifies the condition explicitly for five orbit representatives, with determinants −1,1,2,−1,1, all nonzero for odd q. This is a genuine check, not a circular use of the classification. The twice-odd construction is self-contained: the binary cross block vanishes on non-Fano cuts via the simplex/Hamming code support argument (Eq. (13)), and the odd cross block vanishes on the seven Fano cuts via explicit null-vector certificates (Table II, Eqs. (25)–(29)), with h_t c^T nonzero modulo q. The final split d=2^α m uses the external product property of AME states, cited to both Rains (Ref. [17]) and the authors' own Ref. [18]; because Rains is an independent source, the self-citation is not load-bearing. The power-of-two cases and the Reed–Solomon construction are also cited to external literature, and nonexistence at d=2 is cited to an external result. No fitted parameter is renamed as a prediction; no theorem from the present authors' prior work is invoked to forbid alternatives; no quantity is defined in terms of the target claim. The note about GPT-5.6 assistance is a transparency statement and is followed by independent verification, so it does not introduce circularity. Overall, the derivation chain is self-contained apart from standard, externally corroborated ingredients.

Assumptions & free parameters 1 free parameters · 6 assumptions · 0 invented entities

No unknown parameters are fitted; the only hand choice is the vector c. All other inputs are standard theorems or previously published existence results. The constructions introduce no new physical entities such as particles, forces, or dimensions.

free parameters (1)
  • c = (1,-1,1,0,0,0,0) = (1,-1,1,0,0,0,0)
    Chosen by hand in the twice-odd construction so that h_t c^T is nonzero modulo every odd q for all seven Fano cuts; this forces T_{01}=0 on those cuts and cancels the binary cross terms.
assumptions (6)
  • domain assumption Theorem 3 of Ref. [8]: if for every 3-subset S some Γ_{S,R} with R⊆S^c is invertible over Z_q, then the quadratic-phase state |G_q> is AME.
    Used to conclude Eq. (6) from the five determinant checks. Not proved in the paper.
  • standard math Tensor product of AME(7,d1) and AME(7,d2) is AME(7,d1d2) (Refs. [17,18]).
    Used in the classification case split to combine known prime-power states with odd-dimension states.
  • domain assumption AME(7,4) exists (Refs. [19,20]).
    Covers α=2 in the d=2^α m split.
  • domain assumption A [7,3,5] generalized Reed-Solomon code over F_{2^α}, α≥3, yields an AME(7,2^α) state (Refs. [8,19,22]).
    Covers α≥3 in the case split.
  • domain assumption AME(7,2) does not exist (Ref. [9]).
    Provides the necessity half of the iff classification.
  • standard math The Hamming code D=C∪(C+1) has dual distance 4, so its projection onto any 3 coordinates is uniform; the weight-3 words of C+1 have Fano-plane supports.
    Used in the binary part to derive Eq. (10) and the support restriction Eq. (13); partially verified by Table I.

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Pith. "Pith review of Complete Existence Classification of Seven-Partite Absolutely Maximally Entangled States." pith.science (2026). https://pith.science/paper/P3BLC5DF

@misc{pith2026260801011,
  author       = {Pith},
  title        = {Pith review of: Complete Existence Classification of Seven-Partite Absolutely Maximally Entangled States},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/P3BLC5DF}},
  note         = {Machine review of arXiv:2608.01011}
}
abstract

We prove that an absolutely maximally entangled state of seven qudits exists if and only if the local dimension satisfies $d\geq 3$. Prior to this work, to the best of our knowledge, $\text{AME}(7,d)$ states were known to exist only when $d$ is a prime power other than $2$, or when $d$ can be expressed as a product of dimensions for which existence was already known. Since it has been proved that no $\text{AME}(7,2)$ state exists, it remains to establish existence for all $d\geq 3$. We construct cyclic quadratic-phase states for every odd local dimension and develop a coupled binary--odd-dimensional construction for every dimension congruent to $2$ modulo $4$. Together with the known power-of-two cases and the product property of AME states, these constructions cover every local dimension $d\geq 3$.

Figures

Figures reproduced from arXiv: 2608.01011 by the authors.

Figure 1
Figure 1. FIG. 1. The Fano plane in the cyclic labeling used here. Its [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗

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Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Symmetry-guided constructions of absolutely maximally entangled states in five open cases

    quant-ph 2026-08 conditional novelty 7.0 of 10

    New explicit Hermitian self-dual MDS codes yield AME(12,5), AME(18,11), AME(18,13), and their 17-party projections.

Reference graph

Works this paper leans on

24 extracted references · 22 canonical work pages · cited by 1 Pith paper

  1. [8]

    K. Feng, L. Jin, C. Xing, and C. Yuan, IEEE Transac- tions on Information Theory63, 5618 (2017)

  2. [1]

    Multiplying by the left-null vector gives htcT = (ht)Bt cT Bt = (ht)Bt ΓBt,Lt zT = 0 (modq),(29) which contradicts Eq

    To prove image exclusion, suppose instead thatc T Bt = ΓBt,Lt zT for some row vectorz∈Z Lt q . Multiplying by the left-null vector gives htcT = (ht)Bt cT Bt = (ht)Bt ΓBt,Lt zT = 0 (modq),(29) which contradicts Eq. (27). Hencec T Bt /∈im(ΓBt,Lt ) and T Lt 01 = TrBt |G(q) 0 ⟩⟨G(q) 1 |=0(t∈Z 7).(30) IdentifyC 2q ∼= C2 ⊗C q party by party and set |Ψ2q⟩= |0L⟩|...

  3. [2]

    Helwig, W

    W. Helwig, W. Cui, A. Riera, J. I. Latorre, and H.-K. Lo, Phys. Rev. A86, 052335 (2012)

  4. [3]

    A. J. Scott, Phys. Rev. A69, 052330 (2004)

  5. [4]

    Pastawski, B

    F. Pastawski, B. Yoshida, D. Harlow, and J. Preskill, J. High Energy Phys.2015, 149

  6. [5]

    Huber and M

    F. Huber and M. Grassl, Quantum4, 284 (2020)

  7. [6]

    Alsina and M

    D. Alsina and M. Razavi, Phys. Rev. A103, 022402 (2021)

  8. [7]

    Mazurek, M

    P. Mazurek, M. Farkas, A. Grudka, M. Horodecki, and M. Studzi´ nski, Phys. Rev. A101, 042305 (2020)

Show all 24 references
  1. [9]

    Higuchi and A

    A. Higuchi and A. Sudbery, Phys. Lett. A273, 213 (2000)

  2. [10]

    Horodecki, L

    P. Horodecki, L. Rudnicki, and K. ˙Zyczkowski, PRX Quantum3, 010101 (2022)

  3. [11]

    Then [RS 01]r,s = 1 23 # (u, v)∈C 2 :u S =r,(v+1) S =s, uB = (v+1) B

    = I23 23 ,|S|= 3.(10) For the off-diagonal logical block, letr, s∈Z S 2 . Then [RS 01]r,s = 1 23 # (u, v)∈C 2 :u S =r,(v+1) S =s, uB = (v+1) B . (11) FIG. 1. The Fano plane in the cyclic labeling used here. Its seven triples areL t ={t, t+ 1, t+ 3},t∈Z 7. Suppose that (u, v)∈C...

  4. [12]

    Huber, O

    F. Huber, O. G¨ uhne, and J. Siewert, Phys. Rev. Lett. 118, 200502 (2017)

  5. [13]

    S. A. Rather, A. Burchardt, W. Bruzda, G. Rajchel- Mieldzio´ c, A. Lakshminarayan, and K.˙Zyczkowski, Phys. Rev. Lett.128, 080507 (2022)

  6. [14]

    Huber and N

    F. Huber and N. Wyderka, Table of absolutely maximally entangled states, accessed on 29 Jul., 2026

  7. [15]

    Rajchel-Mieldzio´ c, R

    G. Rajchel-Mieldzio´ c, R. Bistro´ n, A. Rico, A. Lakshmi- narayan, and K. ˙Zyczkowski, Rep. Prog. Phys.89, 057601 (2026)

  8. [16]

    Ball and R

    S. Ball and R. Simoens, Phys. Rev. Lett.137, 050202 (2026)

  9. [17]

    A. M. Steane, Phys. Rev. Lett.77, 793 (1996)

  10. [18]

    A. S. Hedayat, N. J. A. Sloane, and J. Stufken,Orthog- onal arrays: theory and applications(Springer-Verlag, New York, 1999)

  11. [19]

    Rains, IEEE Transactions on Information Theory45, 1827 (1999)

    E. Rains, IEEE Transactions on Information Theory45, 1827 (1999)

  12. [20]

    Shi, M.-S

    F. Shi, M.-S. Li, L. Chen, and X. Zhang, Phys. Rev. A 104, 032601 (2021)

  13. [21]

    Raissi, A

    Z. Raissi, A. Teixid´ o, C. Gogolin, and A. Ac ´ ın, Phys. Rev. Research2, 033411 (2020)

  14. [22]

    Huang, I

    H. Huang, I. Ahmed, D. Zhang, X.-w. Zha, and Y. Zhang, Laser Phys.31, 015201 (2021)

  15. [23]

    F. J. MacWilliams and N. J. A. Sloane,The theory of error-correcting codes(North-Holland Publishing Com- pany, Amsterdam, 1977)

  16. [24]

    Goyeneche and K

    D. Goyeneche and K. ˙Zyczkowski, Phys. Rev. A90, 022316 (2014)

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