- The paper demonstrates methods for constructing new additive MDS twisted Reed–Solomon (ATRS) codes, specifically addressing single-twist with arbitrary hooks and doubly twisted codes, and corrects a parity-check formula error in prior work.
- The study provides precise criteria for MDS conditions through detailed analysis of traces and norms of evaluation points, requiring mathematical induction and assumptions like char$(F_q)$ â§µ r.
- The authors use unique vector characteristics and Schur square analysis to prove ineffectiveness to additive RS codes, concluding these codes exist for certain residue classes and parameters.
Context and contribution
This paper concerns additive twisted Reed–Solomon (ATRS) codes over extension fields Fqr​, i.e., Fq​-linear codes of length n in Fqrn​ obtained by evaluating k-dimensional spaces of "twisted" polynomials over Fq​. Building on the additive generalized Reed–Solomon (AGRS) framework of Yadav–Sharma [sharma2024mds] and the single-twist analysis (t=2, hook h=k−1) of Ma et al. [JiayuMa2026], the authors make three contributions: (i) necessary and sufficient conditions for ATRS codes with twist t=2 and an arbitrary hook to be additive MDS; (ii) the first treatment of doubly twisted additive codes, with twist vector t=(1,2) and hook vector Fq​0; and (iii) a corrected, systematic method for computing parity-check matrices, along the way identifying an error in the parity-check formula of [JiayuMa2026]. Throughout, evaluation points are drawn from Fq​1, one representative per Frobenius orbit of elements with exactly Fq​2 distinct conjugates.
Single-twist codes with arbitrary hook
The first family is Fq​3, spanned over Fq​4 by evaluations of polynomials of degree less than Fq​5 in which the coefficient Fq​6 contributes an extra term Fq​7. Since this space is contained in that of Fq​8, a distance lower bound shows the code is always either additive MDS or additive almost MDS; it is automatically additive MDS whenever Fq​9. For the two exceptional residue classes, the paper gives exact criteria: for n0 the code is additive MDS if and only if n1 for every subset n2 with n3, where n4 is an explicit expression built from elementary symmetric functions of the conjugates n5 and traces n6; for n7, the code is additive almost MDS if and only if n8 and n9 for some Fqrn​0 of size Fqrn​1. These results strictly generalize [JiayuMa2026], which handles only Fqrn​2.
The case Fqrn​3 admits a substantially simpler criterion involving norms rather than general symmetric functions: MDS-ness is equivalent to Fqrn​4 for all Fqrn​5. This simplification enables existence results via explicit counting of special field elements:
- Trace-zero family: assuming Fqrn​6, the paper proves Fqrn​7, where Fqrn​8 collects trace-zero representatives of full-length orbits. The key lemma shows Fqrn​9 has k0 distinct conjugates iff k1 lies in no proper subfield, using an induction on k2 that requires k3 — an assumption on which the resulting existence claim genuinely depends. Taking k4 yields additive MDS codes k5 for every nonzero k6, verified computationally, e.g., a k7 code over k8.
- Norm-one family: analogously, k9 counts norm-one representatives, giving additive MDS codes for all Fq​0 and every Fq​1 when Fq​2, e.g., a Fq​3 code over Fq​4.
The authors emphasize that these lengths exceed those attainable at Fq​5 in prior work — the principal payoff of allowing arbitrary hooks.
Inequivalence to additive RS codes via Schur squares
Monomial equivalence preserves the dimension of the Schur square, while Fq​6. The paper exhibits, in each family, an explicit set of Fq​7 linearly independent Schur products lying in Fq​8, so that Fq​9 whenever t=20 (the independence argument reduces to showing a polynomial of degree t=21 cannot vanish on all t=22 conjugates). Consequently both families contain additive MDS codes not monomially equivalent to any ARS code under the mild condition t=23. The same technique covers the double-twist family.
Double-twisted codes
For t=24, t=25, the twisted space is spanned by t=26. As before, such codes are additive MDS or almost MDS, and are MDS for all t=27. For the exceptional classes, the criteria become: MDS iff t=28 for all t=29; almost-MDS iff h=k−10 and h=k−11 for some h=k−12 of size h=k−13. Existence follows on the same special point sets: over h=k−14 (trace zero), the code is MDS for all pairs h=k−15 when h=k−16; over h=k−17 (norm one), it is MDS whenever h=k−18 and h=k−19. For t=20, a counting argument gives MDS codes whenever t=21. Examples include a t=22 code and an t=23 code over t=24.
Parity-check matrices and correction to prior work
The dual construction uses a vector t=25 with t=26, where t=27 is the full Vandermonde-type matrix up to exponent t=28; the product t=29 is lower-triangular Toeplitz with entries t=(1,2)0. Applying elementary row/column operations eliminates the offending block, yielding an explicit parity-check matrix when t=(1,2)1 for both families. When t=(1,2)2, the paper shows t=(1,2)3 as well (via the minimal polynomial relation), and the dual collapses cleanly: t=(1,2)4.
Notably, the paper demonstrates by counterexample that Theorem 3.6(a) of [JiayuMa2026] is incorrect: applying its formula to a concrete t=(1,2)5 code over t=(1,2)6 produces a matrix t=(1,2)7 with t=(1,2)8, violating the defining property of a parity-check matrix. The corrected procedure here resolves this defect generally.
Limitations and open questions
Several restrictions qualify the results. The automatic MDS dichotomy leaves the residue classes t=(1,2)9 as the only cases requiring conditions, and the counting-based existence arguments need Fq​00. The trace-zero existence result requires Fq​01, and the norm-one family requires Fq​02; whether analogous constructions exist outside these hypotheses is left open. The inequivalence theorem holds only for Fq​03, so short and long codes in these families are not covered. The double-twist analysis is restricted to hooks Fq​04; the general two-hook problem remains untreated, as does the determination of parity-check matrices for arbitrary twist/hook vectors. Finally, the paper notes that extending the additive framework to other TGRS variants may yield further additive MDS families, but does not carry this out.
Conclusion
The paper extends the theory of additive twisted Reed–Solomon codes in two directions: arbitrary hooks for the single twist Fq​05, and a first study of the double-twist case Fq​06. It supplies sharp MDS criteria in terms of traces and norms of evaluation points, constructive existence theorems based on explicit enumeration of trace-zero and norm-one orbit representatives (yielding lengths beyond those previously known for Fq​07), Schur-square proofs of inequivalence to ARS codes, and correct parity-check matrices — including a demonstrated correction to an error in the existing literature [JiayuMa2026].