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IEEE Open Journal of the Communications Society

Singer-Difference-Set Qudit Stabilizer Codes From Non-Degenerate Quadrics in PG( d , q ): Construction, Structural Theorems, and Monte-Carlo Performance

Michel Kulhandjian, Lajos Hanzo

Published Jan 1, 2026• 0 citations
Publisher

Abstract

We propose $\mathcal {Q}(q,d)$ , a new family of $\mathbb {F}_{q}$ -ary non-CSS qudit stabilizer codes parameterised by a prime power $q$ and dimension $d\ge 2$ , constructed from Singer difference sets and non-degenerate quadrics in the projective geometry $\mathop {\mathrm {PG}}\nolimits (d,q)$ . The parity-check matrix $H {\,}\text {=}{\,}(A\mid M_{Q}A)$ couples the Singer-circulant point-hyperplane incidence matrix $A$ with the formal trace-of-square quadric circulant $M_{Q}$ , and a Cancellation Lemma exploits the design-theoretic identity $(k-\lambda){\,}\text {=}{\,}q^{d-1}\equiv 0\pmod p$ to make $H$ symplectic-isotropic over $\mathbb {F}_{q}$ for every $(q,d)$ . The novelty of the construction is concentrated in five original structural theorems: (i) an unconditional cross-correlation modular-constancy theorem $\nu \equiv 1\pmod q$ at $q$ odd, $d\ge 3$ with a sharp two-value pattern $V_{2}-V_{1}{\,}\text {=}{\,}q^{(d-1)/2}$ , proving a 2-torsion distance ceiling; (ii) a Chinese-Remainder-Theorem (CRT) zero-count theorem $\#\{f:\tau _{H,f}{\,}\text {=}{\,}0\}{\,}\text {=}{\,}(|\mathcal {F}|-1)/2$ ; (iii) an explicit Clifford bridge $U_{M}{\,}\text {=}{\,}H^{\otimes n}{\,}\mathrm {CZ}^{(M)}{\,}H^{\otimes n}$ that identifies $\mathcal {Q}(q,2)$ as Clifford-equivalent to a graph-state encoding of the trivial Singer CSS code, with the classical 2021 low-density-spreading (LDS) sign-flip pattern realised by the symmetric circulant $M$ ; (iv) a paired column-rigidity equality $d_{\min }{\,}\text {=}{\,}R_{P}+1$ exactly; and (v) a rigorous lower bound $d_{\min }(\mathcal {Q}(7,2))\ge 8$ from an exhaustive Singer-Frobenius search. Via a Hamada-Smith specialisation we obtain the closed-form logical dimension $k(p,d){\,}\text {=}{\,}\theta _{d}(p)-\binom {p+d-1}{d}-1$ , with the flagship $d{\,}\text {=}{\,}2$ family $\mathcal {Q}(p,2){\,}\text {=}{\,}[[p^{2}+p+1,{\,}p(p+1)/2,{\,}d_{\min }]]_{p}$ attaining asymptotic rate $\tfrac {1}{2}$ . For general odd primes $p\ge 3$ the flagship distance is conjectured to satisfy $d_{\min }(\mathcal {Q}(p,2)){\,}\text {=}{\,}p+1$ ; this conjecture is analytically proven exact at $p{\,}\text {=}{\,}5$ and exhaustively lower-bounded to $d_{\min }\ge 8$ at $p{\,}\text {=}{\,}7$ , and remains open for general $p$ . Concrete instances include $\mathcal {Q}(3,2){\,}\text {=}{\,}[[{13,6,3}]]_{3}$ , $\mathcal {Q}(5,2){\,}\text {=}{\,}[[{31,15,6}]]_{5}$ (double-error correcting), $\mathcal {Q}(7,2){\,}\text {=}{\,}[[57,28,d{\ge }8]]_{7}$ , and $\mathcal {Q}(3,4){\,}\text {=}{\,}[[{121,105,3}]]_{3}$ . Monte-Carlo simulations over $1.5{\times }10^{6}$ trials show that $\mathcal {Q}(5,2)$ achieves a $\sim 70\times $ per-logical-qudit improvement over Steane $[[{7,1,3}]]_{2}$ at depolarising rate $p_{\mathrm {ch}}{\,}\text {=}{\,}10^{-3}$ with zero silent logical errors (the “erase-don’t-mistake” property). We use a textbook bounded-distance decoder throughout, leaving Berlekamp-Massey-style cyclic decoding exploiting the Singer-circulant structure as the natural sequel. A fifteen-row axis-by-axis comparison against the closest prior constructions establishes that the Singer-difference-set + quadric-Gram-matrix combination, together with the closed-form $k$ , the cross-correlation and CRT zero-count theorems, the explicit Clifford bridge to the 2021 LDS construction, and the proven 2-torsion ceiling, is new.

DOI
10.1109/ojcoms.2026.3740294

Related papers

Singer-Difference-Set Qudit Stabilizer Codes from Non-Degenerate Quadrics in PG(d,q)PG(d,q): Construction, Structural Theorems, and Monte-Carlo Performance

Michel Kulhandjian, Lajos Hanzo

We propose Q(q,d), a family of q-ary non-CSS qudit stabilizer codes with prime power q and dimension d >= 2, constructed from Singer difference sets and non-degenerate quadrics in PG(d,q). The parity check H = (A | M_Q A) couples the Singer-circulant incidence matrix A with the quadric circulant M_Q, and a Cancellation Lemma uses the identity (k - lambda) = q^{d-1} = 0 mod p to make H symplectic-isotropic over F_q. Five structural theorems carry the novelty: a cross-correlation modular-constancy identity nu = 1 mod q at q odd, d >= 3, with a two-value pattern that proves a 2-torsion distance ceiling; a CRT zero-count identity; an explicit Clifford bridge identifying Q(q,2) as a graph-state encoding of the trivial Singer CSS code, with the 2021 low-density-spreading (LDS) sign-flip pattern realised by a symmetric circulant; a paired column-rigidity equality d_min = R_P + 1; and a lower bound d_min(Q(7,2)) >= 8 from an exhaustive Singer-Frobenius search. A Hamada-Smith specialisation yields the closed-form logical dimension k(p,d) = theta_d(p) - C(p+d-1, d) - 1, and the flagship Q(p,2) = [[p^2 + p + 1, p(p+1)/2, d_min]]_p attains asymptotic rate one-half. We conjecture d_min(Q(p,2)) = p + 1 for odd primes, proven at p = 5 and lower-bounded to >= 8 at p = 7. Instances include Q(3,2) = [[13,6,3]]_3, Q(5,2) = [[31,15,6]]_5, Q(7,2) = [[57,28, d>=8]]_7, and Q(3,4) = [[121,105,3]]_3. Monte-Carlo over 1.5 x 10^6 trials shows Q(5,2) achieves a 70-fold per-logical-qudit improvement over Steane [[7,1,3]]_2 at depolarising rate 10^-3 with zero silent logical errors. A textbook bounded-distance decoder is used; Berlekamp-Massey-style cyclic decoding is left as the natural sequel.

quant-pharXiv:2610.02392•Oct 5, 2026•0 citations

Quantum XYZ Stabilizer Codes

Alessio Baldelli, Davide Orsucci, Francisco Lázaro +1 more

Stabilizer codes are often constructed within the Calderbank--Shor--Steane (CSS) framework, where two mutually orthogonal binary classical codes define $X$ and $Z$-type stabilizer generators. While this structure is algebraically convenient, additional non-CSS constraints may help suppress low-weight logical operators and improve decoding performance in the finite-length regime. We thus introduce quantum XYZ stabilizer codes, whose parity-check matrix (PCM) is built from three pairwise orthogonal binary PCMs associated with $X$-, $Y$-, and $Z$-type stabilizer generators. A nontrivial point is that an XYZ code instance is not automatically genuinely non-CSS: the same stabilizer group may admit a CSS generating set. We characterize this collapse, obtaining algebraic and rank conditions for deciding when the $Y$-type checks are redundant and when they define genuinely non-CSS stabilizer constraints. We also derive upper and lower bounds on the quantum minimum distance, including bounds for mixed Pauli logical operators. The novel framework includes a known non-CSS topological code, namely the XYZ$^2$ hexagonal code, and yields also sparse finite-length quantum low-density parity-check (qLDPC) constructions from intersecting-subset and quasi-dyadic code families. Simulations under depolarizing code-capacity noise and quaternary belief propagation decoding show that the proposed XYZ qLDPC instances can outperform representative CSS qLDPC instances with similar finite-length parameters.

cs.ITCross-listedarXiv:2607.14988•Jul 17, 2026•0 citations

Minimal Counterexamples of the MacWilliams Extension Theorem for Stabilizer Codes

Ali Assem Mahmoud

The MacWilliams extension theorem fails for module alphabets with non-cyclic socle, and the label alphabet of qudit stabilizer codes, $\F_{q^2}$ over $\F_q$, is such an alphabet. Quantum error correction, however, only ever sees \emph{self-orthogonal} additive codes, and whether that rigidity rescues the theorem---equivalently, whether every weight-preserving isomorphism of stabilizer groups is implemented by local Cliffords and a qudit permutation---was asked by Gluesing-Luerssen and Pllaha and answered negatively by Pllaha for particular qubit codes. We develop the negative answer systematically and at the smallest possible scales. For every prime power $q$ we construct a pair of $[[q+1,q-1]]_q$ stabilizer codes and a weight-preserving isomorphism between them extending to no monomial transformation; the codespaces are inequivalent even under arbitrary local unitaries combined with permutations, though they share Shor--Laflamme enumerators. Self-orthogonality is automatic here, by two elementary lemmas which also show that Dyshko's threshold-length counterexamples were already self-orthogonal, unremarked. For qubits we prove by exhaustive search that length $3$ is minimal and the counterexample essentially unique. Dropping the ``idle qudit'' invariant that detects these, we find the minimal full-support lengths: $4$ for a non-extendable isometry, $5$ for a weight-isometric pair that is not monomially equivalent, realized by explicit $[[5,2]]$ codes; at length $6$ all nontrivial stabilizer elements can have weight $\ge 4$. Whether these codespaces are locally unitarily equivalent is posed as an open problem, connecting the extension problem to the LU--LC circle of questions.

quant-pharXiv:2607.26214•Jul 30, 2026•0 citations

Counting stabiliser codes for arbitrary dimension

Tanmay Singal, Che Chiang, Eugene Hsu +3 more

In this work, we compute the number of [[n,k]]d stabilizer codes made up of d -dimensional qudits, for arbitrary positive integers d . In a seminal work by Gross \cite{Gross2006} the number of [[n,k]]d stabilizer codes was computed for the case when d is a prime (or the power of a prime, i.e., d=pm , but when the qudits are Galois-qudits). The proof in \cite{Gross2006} is inapplicable to the non-prime case. For our proof, we introduce a group structure to [[n,k]]d codes, and use this in conjunction with the Chinese remainder theorem to count the number of [[n,k]]d codes. Our work overlaps with \cite{Gross2006} when d is a prime and in this case our results match exactly, but the results differ for the more generic case. Despite that, the overall order of magnitude of the number of stabilizer codes scales agnostic of whether the dimension is prime or non-prime. This is surprising since the method employed to count the number of stabilizer states (or more generally stabilizer codes) depends on whether d is prime or not. The cardinality of stabilizer states, which was so far known only for the prime-dimensional case (and the Galois qudit prime-power dimensional case) plays an important role as a quantifier in many topics in quantum computing. Salient among these are the resource theory of magic, design theory, de Finetti theorem for stabilizer states, the study and optimisation of the classical simulability of Clifford circuits, the study of quantum contextuality of small-dimensional systems and the study of Wigner-functions. Our work makes available this quantifier for the generic case, and thus is an important step needed to place results for quantum computing with non-prime dimensional quantum systems on the same pedestal as prime-dimensional systems.

arXiv:2209.01449•Quantum•Jul 6, 2023•5 citations

Stabilizer codes from modified symplectic form

Tejas Gandhi, Piyush P. Kurur, Mittal, Rajat

Stabilizer codes form an important class of quantum error correcting codes which have an elegant theory, efficient error detection, and many known examples. Constructing stabilizer codes of length $n$ is equivalent to constructing subspaces of $\mathbb{F}_p^n \times \mathbb{F}_p^n$ which are "isotropic" under the symplectic bilinear form defined by $\left\langle (\mathbf{a},\mathbf{b}),(\mathbf{c},\mathbf{d}) \right\rangle = \mathbf{a}^{\mathrm{T}} \mathbf{d} - \mathbf{b}^{\mathrm{T}} \mathbf{c}$. As a result, many, but not all, ideas from the theory of classical error correction can be translated to quantum error correction. One of the main theoretical contribution of this article is to study stabilizer codes starting with a different symplectic form. In this paper, we concentrate on cyclic codes. Modifying the symplectic form allows us to generalize the previous known construction for linear cyclic stabilizer codes, and in the process, circumvent some of the Galois theoretic no-go results proved there. More importantly, this tweak in the symplectic form allows us to make use of well known error correcting algorithms for cyclic codes to give efficient quantum error correcting algorithms. Cyclicity of error correcting codes is a "basis dependent" property. Our codes are no more "cyclic" when they are derived using the standard symplectic forms (if we ignore the error correcting properties like distance, all such symplectic forms can be converted to each other via a basis transformation). Hence this change of perspective is crucial from the point of view of designing efficient decoding algorithm for these family of codes. In this context, recall that for general codes, efficient decoding algorithms do not exist if some widely believed complexity theoretic assumptions are true.

arXiv:1708.00617•Aug 2, 2017•1 citation

Active Stabilizers In Reed–Muller CSS Codes From Cayley–Dickson Zero-Divisors

Giovanni Levratti

We establish three results connecting the zero-divisor structure of the Cayley–Dickson algebras Aₙ to the stabilizer formalism of quantum error-correcting codes. Step 1 (Bijection, n=4). The 7 lo-flats of ZD(4) — weight-4 subsets {a,b,c,d} ⊂ {1,...,7} with a⊕b⊕c⊕d=0 — are in explicit bijection with the 7 non-identity elements of the X-stabilizer group of the Steane [[7,1,3]] code. All 7 lo-flats carry identical sign-parity pattern: π(EE|FF)=−1 (inactive), π(EF₁)=π(EF₂)=+1 (active). Step 2 (Operator translation). For every mixed flat F={i,j,8+k,8+l} in A₄, the algebraic identity π_A·π_B·π_C=−1 translates into the Clifford-group identity (Z_αZ_β)(X_αX_γ)(X_βX_γ) = −Y_αY_β. The global phase −1 is the precise Clifford avatar of π_Aπ_Bπ_C=−1. The operator −Y_αY_β is a detectable error with full-group syndrome weight 2^(n−2), proved for all n≥4 and verified on QPU. Step 3 (Extension to n=5, verified on QPU). The 15 Fano planes of PG(3,F₂) are in explicit bijection with the 15 non-identity elements of the X-stabilizer group S_X ≅ (Z/2Z)⁴ of the [[15,7,3]] code (4 generators, 2⁴−1=15 non-identity elements). The phase identity and syndrome formula extend to all n≥4 (Universal Phase Lemma). Syndrome structure verified on ibm_kingston (156-qubit QPU, job d8bm67ijki0s73aq6idg, 27 May 2026). The Type-A/Type-B criterion for Fano planes in PG(3,F₂) is resolved: a plane W is Type-B if and only if 8∈W or W={1,...,7}, where 8=(1,0,0,0)∈F₂⁴ is the bridge element between A₃ and A₄ in the Cayley–Dickson tower. All algebraic results are cited from the companion papers (doi:10.5281/zenodo.20315751, doi:10.5281/zenodo.20417859).Every claim is labelled [VERIFIED], [THEOREM], or [OPEN] throughout.

•May 28, 2026•0 citations
We propose Q(q,d)\mathcal {Q}(q,d)Q(q,d) , a new family of Fq\mathbb {F}_{q}Fq​ -ary non-CSS qudit stabilizer codes parameterised by a prime power qqq and dimension d≥2d\ge 2d≥2 , constructed from Singer difference sets and non-degenerate quadrics in the projective geometry PG(d,q)\mathop {\mathrm {PG}}\nolimits (d,q)PG(d,q) . The parity-check matrix H = (A∣MQA)H {\,}\text {=}{\,}(A\mid M_{Q}A)H=(A∣MQ​A) couples the Singer-circulant point-hyperplane incidence matrix AAA with the formal trace-of-square quadric circulant MQM_{Q}MQ​ , and a Cancellation Lemma exploits the design-theoretic identity (k−λ) = qd−1≡0(modp)(k-\lambda){\,}\text {=}{\,}q^{d-1}\equiv 0\pmod p(k−λ)=qd−1≡0(modp) to make HHH symplectic-isotropic over Fq\mathbb {F}_{q}Fq​ for every (q,d)(q,d)(q,d) . The novelty of the construction is concentrated in five original structural theorems: (i) an unconditional cross-correlation modular-constancy theorem ν≡1(modq)\nu \equiv 1\pmod qν≡1(modq) at qqq odd, d≥3d\ge 3d≥3 with a sharp two-value pattern V2−V1 = q(d−1)/2V_{2}-V_{1}{\,}\text {=}{\,}q^{(d-1)/2}V2​−V1​=q(d−1)/2 , proving a 2-torsion distance ceiling; (ii) a Chinese-Remainder-Theorem (CRT) zero-count theorem #{f:τH,f = 0} = (∣F∣−1)/2\#\{f:\tau _{H,f}{\,}\text {=}{\,}0\}{\,}\text {=}{\,}(|\mathcal {F}|-1)/2#{f:τH,f​=0}=(∣F∣−1)/2 ; (iii) an explicit Clifford bridge UM = H⊗n CZ(M) H⊗nU_{M}{\,}\text {=}{\,}H^{\otimes n}{\,}\mathrm {CZ}^{(M)}{\,}H^{\otimes n}UM​=H⊗nCZ(M)H⊗n that identifies Q(q,2)\mathcal {Q}(q,2)Q(q,2) as Clifford-equivalent to a graph-state encoding of the trivial Singer CSS code, with the classical 2021 low-density-spreading (LDS) sign-flip pattern realised by the symmetric circulant MMM ; (iv) a paired column-rigidity equality dmin⁡ = RP+1d_{\min }{\,}\text {=}{\,}R_{P}+1dmin​=RP​+1 exactly; and (v) a rigorous lower bound dmin⁡(Q(7,2))≥8d_{\min }(\mathcal {Q}(7,2))\ge 8dmin​(Q(7,2))≥8 from an exhaustive Singer-Frobenius search. Via a Hamada-Smith specialisation we obtain the closed-form logical dimension k(p,d) = θd(p)−(p+d−1d)−1k(p,d){\,}\text {=}{\,}\theta _{d}(p)-\binom {p+d-1}{d}-1k(p,d)=θd​(p)−(dp+d−1​)−1 , with the flagship d = 2d{\,}\text {=}{\,}2d=2 family Q(p,2) = [[p2+p+1, p(p+1)/2, dmin⁡]]p\mathcal {Q}(p,2){\,}\text {=}{\,}[[p^{2}+p+1,{\,}p(p+1)/2,{\,}d_{\min }]]_{p}Q(p,2)=[[p2+p+1,p(p+1)/2,dmin​]]p​ attaining asymptotic rate 12\tfrac {1}{2}21​ . For general odd primes p≥3p\ge 3p≥3 the flagship distance is conjectured to satisfy dmin⁡(Q(p,2)) = p+1d_{\min }(\mathcal {Q}(p,2)){\,}\text {=}{\,}p+1dmin​(Q(p,2))=p+1 ; this conjecture is analytically proven exact at p = 5p{\,}\text {=}{\,}5p=5 and exhaustively lower-bounded to dmin⁡≥8d_{\min }\ge 8dmin​≥8 at p = 7p{\,}\text {=}{\,}7p=7 , and remains open for general ppp . Concrete instances include Q(3,2) = [[13,6,3]]3\mathcal {Q}(3,2){\,}\text {=}{\,}[[{13,6,3}]]_{3}Q(3,2)=[[13,6,3]]3​ , Q(5,2) = [[31,15,6]]5\mathcal {Q}(5,2){\,}\text {=}{\,}[[{31,15,6}]]_{5}Q(5,2)=[[31,15,6]]5​ (double-error correcting), Q(7,2) = [[57,28,d≥8]]7\mathcal {Q}(7,2){\,}\text {=}{\,}[[57,28,d{\ge }8]]_{7}Q(7,2)=[[57,28,d≥8]]7​ , and Q(3,4) = [[121,105,3]]3\mathcal {Q}(3,4){\,}\text {=}{\,}[[{121,105,3}]]_{3}Q(3,4)=[[121,105,3]]3​ . Monte-Carlo simulations over 1.5×1061.5{\times }10^{6}1.5×106 trials show that Q(5,2)\mathcal {Q}(5,2)Q(5,2) achieves a ∼70×\sim 70\times ∼70× per-logical-qudit improvement over Steane [[7,1,3]]2[[{7,1,3}]]_{2}[[7,1,3]]2​ at depolarising rate pch = 10−3p_{\mathrm {ch}}{\,}\text {=}{\,}10^{-3}pch​=10−3 with zero silent logical errors (the “erase-don’t-mistake” property). We use a textbook bounded-distance decoder throughout, leaving Berlekamp-Massey-style cyclic decoding exploiting the Singer-circulant structure as the natural sequel. A fifteen-row axis-by-axis comparison against the closest prior constructions establishes that the Singer-difference-set + quadric-Gram-matrix combination, together with the closed-form kkk , the cross-correlation and CRT zero-count theorems, the explicit Clifford bridge to the 2021 LDS construction, and the proven 2-torsion ceiling, is new.
We propose Q(q,d), a family of q-ary non-CSS qudit stabilizer codes with prime power q and dimension d >= 2, constructed from Singer difference sets and non-degenerate quadrics in PG(d,q). The parity check H = (A | M_Q A) couples the Singer-circulant incidence matrix A with the quadric circulant M_Q, and a Cancellation Lemma uses the identity (k - lambda) = q^{d-1} = 0 mod p to make H symplectic-isotropic over F_q. Five structural theorems carry the novelty: a cross-correlation modular-constancy identity nu = 1 mod q at q odd, d >= 3, with a two-value pattern that proves a 2-torsion distance ceiling; a CRT zero-count identity; an explicit Clifford bridge identifying Q(q,2) as a graph-state encoding of the trivial Singer CSS code, with the 2021 low-density-spreading (LDS) sign-flip pattern realised by a symmetric circulant; a paired column-rigidity equality d_min = R_P + 1; and a lower bound d_min(Q(7,2)) >= 8 from an exhaustive Singer-Frobenius search. A Hamada-Smith specialisation yields the closed-form logical dimension k(p,d) = theta_d(p) - C(p+d-1, d) - 1, and the flagship Q(p,2) = [[p^2 + p + 1, p(p+1)/2, d_min]]_p attains asymptotic rate one-half. We conjecture d_min(Q(p,2)) = p + 1 for odd primes, proven at p = 5 and lower-bounded to >= 8 at p = 7. Instances include Q(3,2) = [[13,6,3]]_3, Q(5,2) = [[31,15,6]]_5, Q(7,2) = [[57,28, d>=8]]_7, and Q(3,4) = [[121,105,3]]_3. Monte-Carlo over 1.5 x 10^6 trials shows Q(5,2) achieves a 70-fold per-logical-qudit improvement over Steane [[7,1,3]]_2 at depolarising rate 10^-3 with zero silent logical errors. A textbook bounded-distance decoder is used; Berlekamp-Massey-style cyclic decoding is left as the natural sequel.
Stabilizer codes are often constructed within the Calderbank--Shor--Steane (CSS) framework, where two mutually orthogonal binary classical codes define XXX and ZZZ-type stabilizer generators. While this structure is algebraically convenient, additional non-CSS constraints may help suppress low-weight logical operators and improve decoding performance in the finite-length regime. We thus introduce quantum XYZ stabilizer codes, whose parity-check matrix (PCM) is built from three pairwise orthogonal binary PCMs associated with XXX-, YYY-, and ZZZ-type stabilizer generators. A nontrivial point is that an XYZ code instance is not automatically genuinely non-CSS: the same stabilizer group may admit a CSS generating set. We characterize this collapse, obtaining algebraic and rank conditions for deciding when the YYY-type checks are redundant and when they define genuinely non-CSS stabilizer constraints. We also derive upper and lower bounds on the quantum minimum distance, including bounds for mixed Pauli logical operators. The novel framework includes a known non-CSS topological code, namely the XYZ2^22 hexagonal code, and yields also sparse finite-length quantum low-density parity-check (qLDPC) constructions from intersecting-subset and quasi-dyadic code families. Simulations under depolarizing code-capacity noise and quaternary belief propagation decoding show that the proposed XYZ qLDPC instances can outperform representative CSS qLDPC instances with similar finite-length parameters.
The MacWilliams extension theorem fails for module alphabets with non-cyclic socle, and the label alphabet of qudit stabilizer codes, $\F_{q^2}$ over $\F_q$, is such an alphabet. Quantum error correction, however, only ever sees \emph{self-orthogonal} additive codes, and whether that rigidity rescues the theorem---equivalently, whether every weight-preserving isomorphism of stabilizer groups is implemented by local Cliffords and a qudit permutation---was asked by Gluesing-Luerssen and Pllaha and answered negatively by Pllaha for particular qubit codes. We develop the negative answer systematically and at the smallest possible scales. For every prime power qqq we construct a pair of [[q+1,q−1]]q[[q+1,q-1]]_q[[q+1,q−1]]q​ stabilizer codes and a weight-preserving isomorphism between them extending to no monomial transformation; the codespaces are inequivalent even under arbitrary local unitaries combined with permutations, though they share Shor--Laflamme enumerators. Self-orthogonality is automatic here, by two elementary lemmas which also show that Dyshko's threshold-length counterexamples were already self-orthogonal, unremarked. For qubits we prove by exhaustive search that length 333 is minimal and the counterexample essentially unique. Dropping the ``idle qudit'' invariant that detects these, we find the minimal full-support lengths: 444 for a non-extendable isometry, 555 for a weight-isometric pair that is not monomially equivalent, realized by explicit [[5,2]][[5,2]][[5,2]] codes; at length 666 all nontrivial stabilizer elements can have weight ≥4\ge 4≥4. Whether these codespaces are locally unitarily equivalent is posed as an open problem, connecting the extension problem to the LU--LC circle of questions.
In this work, we compute the number of [[n,k]]d stabilizer codes made up of d -dimensional qudits, for arbitrary positive integers d . In a seminal work by Gross \cite{Gross2006} the number of [[n,k]]d stabilizer codes was computed for the case when d is a prime (or the power of a prime, i.e., d=pm , but when the qudits are Galois-qudits). The proof in \cite{Gross2006} is inapplicable to the non-prime case. For our proof, we introduce a group structure to [[n,k]]d codes, and use this in conjunction with the Chinese remainder theorem to count the number of [[n,k]]d codes. Our work overlaps with \cite{Gross2006} when d is a prime and in this case our results match exactly, but the results differ for the more generic case. Despite that, the overall order of magnitude of the number of stabilizer codes scales agnostic of whether the dimension is prime or non-prime. This is surprising since the method employed to count the number of stabilizer states (or more generally stabilizer codes) depends on whether d is prime or not. The cardinality of stabilizer states, which was so far known only for the prime-dimensional case (and the Galois qudit prime-power dimensional case) plays an important role as a quantifier in many topics in quantum computing. Salient among these are the resource theory of magic, design theory, de Finetti theorem for stabilizer states, the study and optimisation of the classical simulability of Clifford circuits, the study of quantum contextuality of small-dimensional systems and the study of Wigner-functions. Our work makes available this quantifier for the generic case, and thus is an important step needed to place results for quantum computing with non-prime dimensional quantum systems on the same pedestal as prime-dimensional systems.
Stabilizer codes form an important class of quantum error correcting codes which have an elegant theory, efficient error detection, and many known examples. Constructing stabilizer codes of length nnn is equivalent to constructing subspaces of Fpn×Fpn\mathbb{F}_p^n \times \mathbb{F}_p^nFpn​×Fpn​ which are "isotropic" under the symplectic bilinear form defined by ⟨(a,b),(c,d)⟩=aTd−bTc\left\langle (\mathbf{a},\mathbf{b}),(\mathbf{c},\mathbf{d}) \right\rangle = \mathbf{a}^{\mathrm{T}} \mathbf{d} - \mathbf{b}^{\mathrm{T}} \mathbf{c}⟨(a,b),(c,d)⟩=aTd−bTc. As a result, many, but not all, ideas from the theory of classical error correction can be translated to quantum error correction. One of the main theoretical contribution of this article is to study stabilizer codes starting with a different symplectic form. In this paper, we concentrate on cyclic codes. Modifying the symplectic form allows us to generalize the previous known construction for linear cyclic stabilizer codes, and in the process, circumvent some of the Galois theoretic no-go results proved there. More importantly, this tweak in the symplectic form allows us to make use of well known error correcting algorithms for cyclic codes to give efficient quantum error correcting algorithms. Cyclicity of error correcting codes is a "basis dependent" property. Our codes are no more "cyclic" when they are derived using the standard symplectic forms (if we ignore the error correcting properties like distance, all such symplectic forms can be converted to each other via a basis transformation). Hence this change of perspective is crucial from the point of view of designing efficient decoding algorithm for these family of codes. In this context, recall that for general codes, efficient decoding algorithms do not exist if some widely believed complexity theoretic assumptions are true.
We establish three results connecting the zero-divisor structure of the Cayley–Dickson algebras Aₙ to the stabilizer formalism of quantum error-correcting codes. Step 1 (Bijection, n=4). The 7 lo-flats of ZD(4) — weight-4 subsets {a,b,c,d} ⊂ {1,...,7} with a⊕b⊕c⊕d=0 — are in explicit bijection with the 7 non-identity elements of the X-stabilizer group of the Steane [[7,1,3]] code. All 7 lo-flats carry identical sign-parity pattern: π(EE|FF)=−1 (inactive), π(EF₁)=π(EF₂)=+1 (active). Step 2 (Operator translation). For every mixed flat F={i,j,8+k,8+l} in A₄, the algebraic identity π_A·π_B·π_C=−1 translates into the Clifford-group identity (Z_αZ_β)(X_αX_γ)(X_βX_γ) = −Y_αY_β. The global phase −1 is the precise Clifford avatar of π_Aπ_Bπ_C=−1. The operator −Y_αY_β is a detectable error with full-group syndrome weight 2^(n−2), proved for all n≥4 and verified on QPU. Step 3 (Extension to n=5, verified on QPU). The 15 Fano planes of PG(3,F₂) are in explicit bijection with the 15 non-identity elements of the X-stabilizer group S_X ≅ (Z/2Z)⁴ of the [[15,7,3]] code (4 generators, 2⁴−1=15 non-identity elements). The phase identity and syndrome formula extend to all n≥4 (Universal Phase Lemma). Syndrome structure verified on ibm_kingston (156-qubit QPU, job d8bm67ijki0s73aq6idg, 27 May 2026). The Type-A/Type-B criterion for Fano planes in PG(3,F₂) is resolved: a plane W is Type-B if and only if 8∈W or W={1,...,7}, where 8=(1,0,0,0)∈F₂⁴ is the bridge element between A₃ and A₄ in the Cayley–Dickson tower. All algebraic results are cited from the companion papers (doi:10.5281/zenodo.20315751, doi:10.5281/zenodo.20417859).Every claim is labelled [VERIFIED], [THEOREM], or [OPEN] throughout.