---
title: Graded Quantum Codes
url: https://www.emergentmind.com/topics/graded-quantum-codes
type: topic
---

# Graded Quantum Codes

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Graded quantum codes are quantum error-correcting codes equipped with an explicit grading that organizes either the algebraic data used to construct the code or the local Hilbert-space structure on which the code is defined. In one formulation, a graded quantum code is a stabilizer/CSS quantum code whose classical and/or homological ingredients share an explicit grading: on the weighted algebraic geometry side, codes come from evaluating graded polynomials on rational points of weighted projective hypersurfaces, while on the homological side, codes arise from chain complexes of graded vector spaces or graded modules, possibly with torsion [2508.07542]. In another formulation, graded quantum codes are mixed-alphabet quantum error-correcting codes, in which the physical subsystems have differing local dimensions and the grading is by local dimension [1205.4253]. These two usages are not identical in construction, but both treat grading as a structural device that refines parameters, constraints, and decoding.

## 1. Conceptual scope and definitions

In the weighted-algebraic and homological framework, a graded quantum code is a stabilizer/CSS quantum code whose classical and/or homological ingredients share an explicit grading [2508.07542]. Two complementary instances are developed. The first is the weighted algebraic geometry side, where codes come from evaluating graded, weighted-homogeneous polynomials on rational points of hypersurfaces in weighted projective spaces over finite fields. The grading is the weighted degree of monomials and polynomials, and it interacts with orbifold singularities. The second is the homological side, where codes arise from chain complexes
$$
C_2 \to C_1 \to C_0
$$
of graded vector spaces, and more generally graded modules, possibly with torsion, where the boundary maps respect degree and yield LDPC stabilizer codes via the $\partial$-maps [2508.07542].

The key unifying innovation in this framework is a shared grading across code components. On the algebraic geometry side, the weight grading of coordinates and polynomials controls point counts, dimensions, and self-orthogonality conditions for CSS constructions. On the homological side, the chain-complex grading, possibly multi-graded, with torsion, controls sparsity and the ranks of homology groups used to define quantum parameters. This shared grading enables a refined Singleton-type bound that tightens the standard quantum Singleton bound by an explicit positive correction term $\epsilon$ reflecting entropy or defect contributions from orbifold singularities or graded twisted sectors [2508.07542].

In the mixed-alphabet formulation, graded quantum codes are codes defined over physical subsystems of differing local dimensions, and they are precisely the mixed-alphabet quantum error-correcting codes introduced in "Quantum Error-Correcting Codes over Mixed Alphabets" [1205.4253]. A mixed-alphabet code on $n$ physical subsystems whose local dimensions are not uniform is denoted by
$$
((n,K,d))_{q_1^{n_1} q_2^{n_2}\dots},
$$
or more generally by
$$
((n,K,d))_{p_1 p_2 \dots p_n}.
$$
Here $n$ is the number of physical subsystems, $K$ is the dimension of the code subspace, and $d$ is the code distance; the code detects all errors of weight $< d$ and corrects all errors of weight $\le \lfloor (d-1)/2 \rfloor$ [1205.4253].

A plausible implication is that the term "graded quantum codes" functions as an umbrella for at least two structurally different, but conceptually related, uses of grading: grading by weighted degree or homological degree in code construction, and grading by local subsystem dimension in code representation.

## 2. Weighted algebraic geometry constructions

The weighted algebraic geometry construction begins with a weighted projective space. Let $w=(w_0,\dots,w_m)$ be positive integers with $\gcd(w_0,\dots,w_m)=1$; such a weight vector is well-formed. The weighted projective space over a field $F$ is
$$
\mathbb{P}(w_0,\dots,w_m) = (\mathbb{A}^{m+1}\setminus\{0\})/\mathbb{G}_m,
$$
where $\lambda \in F^\*$ acts by
$$
\lambda \cdot (x_0,\dots,x_m) = (\lambda^{w_0}x_0,\dots,\lambda^{w_m}x_m).
$$
Its homogeneous coordinate ring is $S=F[x_0,\dots,x_m]$, graded by $\deg(x_i)=w_i$, with graded pieces $S_d$ consisting of weighted homogeneous polynomials of total weighted degree $d$ [2508.07542].

A weighted homogeneous polynomial $F\in S_D$ satisfies
$$
F(\lambda^{w_0}x_0,\dots,\lambda^{w_m}x_m)=\lambda^D F(x_0,\dots,x_m),
$$
and the weighted hypersurface
$$
X=V(F)\subset \mathbb{P}(w_0,\dots,w_m)
$$
is the vanishing locus of $F$, defined over $\mathbb{F}_q$ when the coefficients lie in $\mathbb{F}_q$ [2508.07542]. Over $\mathbb{F}_q$, rational points of $\mathbb{P}(w)$ are orbits of $\mathbb{F}_q^\*$ acting by weighted scaling on $\mathbb{A}^{m+1}(\mathbb{F}_q)\setminus\{0\}$. With support $S\subseteq\{0,\dots,m\}$ equal to the indices of nonzero coordinates, the stabilizer has order $\gcd(k_S,q-1)$ with $k_S=\gcd(w_i:i\in S)$. The point count on the ambient space is
$$
|\mathbb{P}(w)(\mathbb{F}_q)|=\sum_{\varnothing\neq S\subseteq\{0,\dots,m\}} (q-1)^{|S|-1}\gcd(k_S,q-1).
$$
For hypersurfaces $X=V(F)$, one stratifies by $S$ and restricts to the zero-locus of $F$ on each stratum [2508.07542].

Classical evaluation codes are constructed by evaluating a finite-dimensional subspace of functions on a set of $n$ rational points:
$$
C(X,L,P)=\{(f(P_1),\dots,f(P_n)):f\in L\}\subset \mathbb{F}_q^n.
$$
Here $L$ is often a graded piece $S_d$ or a Riemann–Roch space $L(D)$ on a curve embedded in a weighted projective space. Weighting and orbifold singularities affect both the dimension and the zero counts, which later determine the quantum CSS parameters [2508.07542].

For the explicit evaluation code
$$
C(X,d)=\mathrm{im}(\mathrm{ev}_d:S_d\to \mathbb{F}_q^m),
$$
with $m=|X(\mathbb{F}_q)|$, the dimension is
$$
k=\dim(\mathrm{im}\,\mathrm{ev}_d)=\dim S_d-\dim I(\mathcal{P})_d,
$$
where $I(\mathcal{P})$ is the weighted vanishing ideal. The minimum distance satisfies
$$
d_{\text{classical}} = m-\max_{f\in S_d\setminus\{0\}} |Z(f)|,
$$
and can be bounded using weighted footprint or Gröbner techniques, adjusting zero multiplicities by stabilizers $\gcd(k_S,q-1)$ [2508.07542].

The CSS lift proceeds when a classical code $C\subseteq C^\perp$ under the Euclidean or Hermitian inner product. In that case, CSS yields a quantum code with parameters
$$
[[n,k_Q,d_Q]], \qquad n=m,\qquad k_Q=n-2k_{\text{classical}},
$$
and
$$
d_Q \ge \min(d_{\text{classical}}, d_{C^\perp}).
$$
In matrix form, for parity-check matrices $H_X,H_Z$, the orthogonality condition is
$$
H_X H_Z^T = 0.
$$
Self-orthogonality can be achieved by choosing degrees or divisors respecting weighted symmetry, residues, or automorphisms; weighted degrees and the canonical class control when $C\subseteq C^\perp$ holds [2508.07542].

A heuristic weighted analogue of Riemann–Roch is
$$
l(D)-l(K-D)=\deg_w(D)+1-g_w,
$$
where $l(\cdot)=\dim L(\cdot)$, $K$ is the canonical divisor, $\deg_w(D)$ is the weighted degree, and $g_w$ is the weighted orbifold genus. Singularities and orbifold points introduce correction terms that affect $l(D)$ and thus $k$ and $d$; in practice one uses that $\dim L(D)\approx \deg_w(D)+1-g_w$ when $\deg_w(D)>2g_w-2$, adjusted for orbifold defects [2508.07542].

## 3. Homological chain-complex and LDPC formulations

The homological formulation generalizes homological quantum codes to graded complexes and modules with torsion [2508.07542]. Let
$$
C_2 \xrightarrow{\partial_2} C_1 \xrightarrow{\partial_1} C_0
$$
be a chain complex over $\mathbb{F}_q$ with boundary maps preserving grading, possibly multi-grading. One defines CSS matrices by
$$
H_X=\partial_1,\qquad H_Z=\partial_2^T,
$$
so that
$$
H_X H_Z^T=\partial_1\partial_2=0.
$$
This realizes the CSS orthogonality relation through functoriality of the boundary [2508.07542].

The resulting quantum code parameters are specified homologically:
$$
n=\dim C_1,
$$
$$
k=\dim H_1(C)=\dim(\ker \partial_1/\mathrm{im}\,\partial_2),
$$
and $d$ is the minimum weight of nontrivial cycles or cochains representing undetectable $X/Z$ errors [2508.07542]. The LDPC property arises when each boundary involves bounded numbers of cells, producing sparse rows and columns. Grading, including bigrading and orbifold sectors, induces block structure in Tanner graphs and constrains sparsity [2508.07542].

Multiple gradings and torsion are central in this formulation. Multiple gradings, as in Khovanov-type complexes or orbifold homology, split the complex into graded sectors which can be filtered to define codes with targeted sparsity and rank. Torsion in homology, including examples associated with rotor models or orbifold fixed loci, contributes logical operators and can alter $k$ and $d$ via additional graded sectors [2508.07542]. The paper explicitly states that torsion homology $H_1^{\mathrm{tors}}(C)$ may carry logical operators with special algebra, and that multi-grading lets one filter complexes to tune $k$ and $d$ [2508.07542].

This homological construction links graded quantum codes to topological and categorical invariants. Examples in the source material include toric surface codes, Khovanov homology codes, and rotor codes with torsion grading [2508.07542]. This suggests that grading functions not merely as book-keeping, but as a mechanism for sector decomposition, sparsity control, and parameter tuning in LDPC stabilizer design.

## 4. Mixed alphabets as grading by local dimension

The mixed-alphabet framework treats grading as heterogeneity in local Hilbert-space dimension [1205.4253]. For a single $l$-level system, generalized Pauli operators are defined by
$$
X_l = \sum_{j\in \mathbb{Z}_l} |j+1 \bmod l\rangle \langle j|,\qquad
Z_l = \sum_{j\in \mathbb{Z}_l} \omega_l^j |j\rangle\langle j|,\qquad
\omega_l=e^{2\pi i/l},
$$
with
$$
Z_l X_l = \omega_l X_l Z_l,\qquad X_l^l = Z_l^l = I.
$$
On a heterogeneous register with local dimensions $\{p_i\}$, the Pauli-type error set is
$$
E=\left\{ \bigotimes_{i=1}^n X_{p_i}^{a_i} Z_{p_i}^{b_i}\mid a_i,b_i\in \mathbb{Z}_{p_i}\right\}.
$$
The support of an error at site $i$ is defined by $(a_i,b_i)\neq (0,0)$, and its weight is the size of the support [1205.4253].

The Knill–Laflamme condition takes the standard form adapted to the heterogeneous Pauli basis. For an encoding projector $P$ onto a $K$-dimensional subspace, the code detects all errors of weight $<d$ if for every such error $E$,
$$
P E P = \lambda_E P
$$
for some scalar $\lambda_E$. The distance $d$ is the smallest weight of an error for which the detection condition fails [1205.4253].

Two construction paradigms are developed. In the reducible case $q=rp$, where one alphabet factors, a $q$-level subsystem can be represented as a composite of a $p$-level and an $r$-level subsystem. The construction then uses a composite coding clique based on graph states over $\mathbb{Z}_p$ and $\mathbb{Z}_r$ [1205.4253]. For a $\mathbb{Z}_p$-weighted graph $G_p=(V,\Gamma_p)$, the graph state is
$$
|\Gamma_p\rangle = \left[\prod_{a,b\in V} U_{ab}^{\Gamma_{ab}}\right] |\theta_0\rangle^{\otimes n},
$$
with
$$
|\theta_0\rangle=(1/\sqrt{p})\sum_{j\in \mathbb{Z}_p}|j\rangle,
$$
and stabilizer generators
$$
g_p(u)=X_p^u Z_p^{u\cdot \Gamma_p},\qquad u\in \mathbb{Z}_p^{\otimes n}.
$$
Similarly, one defines $|\Gamma_r\rangle$ and $g_r(u')$ on the $r$-level subsystem [1205.4253].

The mixed-alphabet basis is then
$$
\left\{ Z_p^c |\Gamma_p\rangle \otimes Z_r^{c'} |\Gamma_r\rangle \mid c\in \mathbb{Z}_p^{\otimes n},\; c'\in \mathbb{Z}_r^{\otimes n_1}\right\}.
$$
A composite coding clique $C_d^K=\{c_i\otimes c_i'\}_{i=1}^K$ is defined through the $d$-uncoverable set $D_d$ and the $d$-purity set $S_d$, together with three conditions: $0\otimes 0\in C_d^K$; for all $s\otimes s'\in S_d$ and all $c\otimes c'\in C_d^K$, one has $\omega_p^{s\cdot c}\omega_r^{s'\cdot c'}=1$; and for all distinct $i,j$, $(c_i-c_j)\otimes(c_i'-c_j')\in D_d$ [1205.4253]. The corresponding code basis is
$$
\{|\psi_{c,c'}\rangle = Z_p^c |\Gamma_p\rangle \otimes Z_r^{c'} |\Gamma_r\rangle \mid (c\otimes c')\in C_d^K\},
$$
and the resulting subspace is a mixed-alphabet code $((n,K,d))_{q^{n_1}p^{n_2}}$ [1205.4253].

When $p$ and $q$ are coprime, the composite coding clique approach is unavailable. The alternative is projection-based construction. One embeds the mixed-alphabet register into an ancillary $n$-quqit register and defines
$$
\mathcal{P}=I_1\otimes \cdots \otimes I_{n_1}\otimes P_{n_1+1}\otimes \cdots \otimes P_n,
$$
where each $P_i$ projects a $q$-level subsystem down to a $p$-level subspace and $\mathrm{Tr}\,P_i=p$ [1205.4253]. If an ancillary $K$-dimensional subspace spanned by $\{|l\rangle\}$ can detect or correct the projected errors $\{\mathcal{P}^\dagger E \mathcal{P}\}$ for all mixed-register errors of weight $<d$, then the normalized projected states
$$
|l'\rangle = \mathcal{P}|l\rangle/\sqrt{\langle l|\mathcal{P}|l\rangle}
$$
define a mixed-alphabet QECC $((n,K,d))_{q^{n_1}p^{n_2}}$ [1205.4253].

## 5. Bounds and parameter relations

The weighted/homological graded framework proposes a refined Singleton bound
$$
d \le \frac{n-k+2}{2} - \frac{\epsilon}{2},
$$
where $\epsilon>0$ quantifies entropy or defect reduction due to grading-compatible orbifold singularities on the weighted algebraic geometry side or twisted homological sectors on the chain-complex side [2508.07542]. In the paper, for quotient or orbifold points $p$ with stabilizer $G_p$,
$$
\epsilon = \frac{1}{2}\sum_p \left(1-\frac{1}{|G_p|}\right).
$$
On weighted AG hypersurfaces, $\epsilon$ reflects Chen–Ruan orbifold cohomology contributions from twisted sectors; on homological codes with orbifold grading, $\epsilon$ counts twisted-sector ranks in orbifold homology or $K$-theory, tightening entropy inequalities [2508.07542].

The validity of this refined bound is limited in scope. It is partially validated for simple $\mathbb{P}^1$-orbifolds, requires a shared grading alignment and mild singularities such as simple quotient singularities, and is supported by heuristic entropy derivations using TQFT defect sectors. A rigorous coding-theoretic proof remains open [2508.07542]. Other bounds discussed in the same framework include Gilbert–Varshamov-type existence bounds for AG codes with weighting, zeta-function or Weil-type bounds controlling $|X(\mathbb{F}_q)|$, and Hamming or Plotkin variants in which polytope footprint methods are modified by grading [2508.07542].

The mixed-alphabet framework establishes a different generalized quantum Singleton bound. For a mixed-alphabet QECC $((n,K,d))_{p_1p_2\dots p_n}$ and any partition $V=A\cup B\cup C$ with $|A|=|B|=d-1$ and $|C|=n-2(d-1)$, one has
$$
K \le \prod_{i\in C} p_i.
$$
Optimizing over all subsets $C$ of size $n-2(d-1)$ yields
$$
K \le \min_{|C|=n-2(d-1)} \prod_{i\in C} p_i.
$$
In the uniform case $p_i=q$ for all $i$, this reduces to
$$
K \le q^{n-2(d-1)},
$$
and for stabilizer codes with $K=q^k$, to the familiar quantum Singleton bound
$$
n-k \ge 2(d-1)
$$
[1205.4253].

The two bounds address different notions of grading. The refined bound with $\epsilon$ modifies the standard Singleton inequality through geometric or homological defect data [2508.07542]. The mixed-alphabet bound modifies the capacity term through the product of local subsystem dimensions [1205.4253]. This suggests that grading can alter code limitations either through defect-sensitive entropy corrections or through heterogeneity in local alphabet size.

## 6. Representative examples and constructions

The weighted algebraic geometry pathway includes several worked examples over small fields [2508.07542]. In one example, a hypersurface in $\mathbb{P}(2,4,6,10)$ over $\mathbb{F}_5$ is defined by
$$
F = x_0^{10}+x_1^5+x_2^2+x_3
$$
of weighted degree $20$. Stratifying by supports and stabilizers yields $|X(\mathbb{F}_5)|=112$. Taking $S_{20}$ gives $\dim S_{20}=\mathrm{den}(20;2,4,6,10)=20$, and choosing a self-orthogonal subspace $L\subseteq S_{20}$ of dimension $k_{\text{classical}}=10$ produces a classical code with parameters $[112,10,d_C]$. The CSS lift gives
$$
[[112,112-2\cdot 10,d_Q]]=[[112,92,d_Q]],
$$
with
$$
d_Q \ge \min(d_C,d_{C_L^\perp}).
$$
Using local stabilizers of orders $\{2,4,6,10\}$, the refined bound gives
$$
d_Q \le (112-92+2)/2-\epsilon/2 = 12-\epsilon/2
$$
for positive but modest $\epsilon$ [2508.07542].

A second example uses the genus-2 curve
$$
y^2=x^5-2x^3+x^2+1
$$
homogenized in $\mathbb{P}(1,1,3)$ over $\mathbb{F}_9$ as
$$
y^2=x^5-2x^3z^2+x^2z^3+z^5.
$$
Using $8$ rational places and a divisor $G$ of degree $5$ yields a classical self-orthogonal AG code with parameters $[8,3,5]$, and the CSS lift gives
$$
[[8,8-2\cdot 3,\ge 5]]=[[8,2,\ge 5]]
$$
[2508.07542]. A third weighted-projective example reports a CSS code $[[10,2,3]]$ over $\mathbb{F}_7$ from a genus-$1$ weighted projective curve in $\mathbb{P}(1,2,3)$ [2508.07542].

The homological pathway includes the toric surface code on an $L\times L$ torus, with parameters
$$
[[2L^2,2,L]],
$$
where $n=\dim C_1=2L^2$, $k=\dim H_1=2$, and $d$ is the shortest nontrivial cycle length $L$ [2508.07542]. A bigraded Khovanov homology code is reported with parameters $[[10,3,4]]$, obtained by filtering the complex $C^{i,j}$ to $C^{\le J}=\bigoplus_{j\le J} C^{*,j}$ [2508.07542]. A rotor code with torsion grading on a $4\times 4$ rotor lattice has $n=32$ sites and parameters
$$
[[32,3,4]],
$$
with $H_1$ rank $2$ plus torsion contributing one logical qubit; the paper gives $\epsilon \approx 1$, leading to
$$
d \le (32-3+2)/2 - 1/2 = 15.5
$$
[2508.07542].

The mixed-alphabet literature provides optimal and suboptimal examples [1205.4253]. The code
$$
((6,8,3))_{4^5 2^1}
$$
is optimal because the generalized Singleton bound gives $K\le 8$ and the construction achieves $K=8$ [1205.4253]. Likewise,
$$
((6,4,3))_{4^4 2^2}
$$
is optimal with $K=4$, and
$$
((5,16,2))_{4^3 2^2}
$$
is optimal via stabilizer pasting, with the bound giving $K\le 16$ and the construction achieving $K=16$ [1205.4253]. By contrast,
$$
((5,9,2))_{3^4 2^1}
$$
constructed via projection is suboptimal, since the bound gives $K\le 18$ but the realized code has $K=9$; the suboptimality is attributed to the fact that the projected errors expand into several Pauli-type operators that must all be detected separately [1205.4253].

The paper also shows that mixed-alphabet methods inform standard uniform constructions, including the optimal code
$$
((6,16,3))_4
$$
and the optimal distance-$2$ families
$$
((2n+3,4^{2n+1},2))_4,\qquad ((2n+3,8^{2n+1},2))_8,
$$
as well as optimal
$$
((2n+3,p^{2n+1},2))_p
$$
for any $p=4k$ when combined with known odd-prime-dimension families [1205.4253].

## 7. Decoding, applications, limitations, and open questions

For weighted AG/CSS codes, decoding is described in terms of syndrome-based algebraic methods [2508.07542]. One measures stabilizers or parity checks derived from evaluation maps or vanishing ideals and then solves for the error through algebraic relations. On curves, Riemann–Roch-based decoders, Berlekamp–Welch-like methods for general evaluation codes, Kötter–Vardy soft-decision approaches, and Sudan-style list decoding can be adapted to weighted settings by respecting weighted degrees and orbit stabilizers in Gröbner computations [2508.07542]. The Hermitian inner product over $\mathbb{F}_{q^2}$ can simplify dual-containing checks, stabilizer generation, and decoding tables [2508.07542]. Parity-check matrices inherit block structures by weighted degree, and Tanner graphs reflect orbit decompositions, potentially aiding iterative decoding [2508.07542].

For homological LDPC codes, the listed decoding methods include iterative belief propagation on Tanner graphs derived from sparse $\partial$-maps, union-find-like decoders for surface or toric generalizations, and minimum-weight perfect matching for planar-like embeddings [2508.07542]. Grading gives multi-layer graphs with structured priors, can localize defects and prioritize correction along graded sectors, and torsion sectors require careful handling because of logical degeneracy [2508.07542]. The source further states that homological LDPC structures often admit near-linear-time decoders and favorable thresholds, and that grading improves locality and message-passing efficacy by partitioning constraints [2508.07542].

The applications identified for the weighted/homological framework are post-quantum cryptography, fault-tolerant quantum computing, and optimization via graded neural networks [2508.07542]. In post-quantum cryptography, graded AG/CSS codes provide structured, high-rate codes whose parameters can be tuned via weighted heights and zeta-function point counts, and grading aids parameter selection and key-size optimization [2508.07542]. In fault-tolerant quantum computing, graded LDPC homological codes offer sparse checks and topological protection; grading aligns with transversal operations or subsystem variants by sectoring stabilizers and logical operators, while orbifold defects $\epsilon$ relate to enhanced syndrome distinguishability and potentially improved thresholds [2508.07542]. For optimization, graded structures enable machine-learning-based parameter search guided by height zeta functions and Hilbert functions to balance $n$, $k$, and $d$ [2508.07542].

The mixed-alphabet framework is motivated by hardware heterogeneity. Multi-level systems such as ququarts and qutrits may co-exist with qubits, higher excited states may be controllable on some sites but not others, and different modules may expose different native dimensions. Mixed-alphabet, hence graded, codes respect this heterogeneity without forcing uniformity [1205.4253]. Decoding proceeds via syndrome extraction from the stabilizers of the underlying graph states or from projections; the syndrome spaces are graded by local dimensions, but the algebra of generalized Pauli operators preserves the standard Knill–Laflamme logic [1205.4253].

Several limitations and open problems remain. In the weighted/homological setting, the refined bound is only partially established for simple orbifold lines, and a general rigorous proof for higher-dimensional weighted hypersurfaces and arbitrary homological gradings is open [2508.07542]. Determining families that meet the refined bound, understanding interaction with asymptotic bounds such as Tsfasman–Vladut–Zink in the quantum setting, developing robust decoders exploiting bigrading and torsion, and building efficient pipelines for weighted point counts, height zeta functions, Gröbner bases in weighted rings, and verification of self-orthogonality are all identified as open directions [2508.07542]. In the mixed-alphabet setting, clique search is NP-complete, stabilizer pasting is shown for distance $2$ but not extended to $d\ge 3$, and projector choice in the coprime case remains difficult because projected errors may expand into many independent Pauli constraints [1205.4253].

Taken together, these results show that graded quantum codes form a technically diverse domain in which grading can organize algebraic geometry data, homological sectors, torsion, or local subsystem dimensions. The common consequence is a refinement of code construction and parameter analysis beyond the ungraded stabilizer setting, with explicit formulas, constructions, and examples already available in both the weighted/homological framework [2508.07542] and the mixed-alphabet framework [1205.4253].

Source: https://www.emergentmind.com/topics/graded-quantum-codes