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arXiv:1604.07925 · Linear Algebra and its Applications

Permutation-invariant qudit codes from polynomials

Yingkai Ouyang

Published Jun 27, 2017• 38 citations
arXivHTMLPDF
DOI
10.1016/j.laa.2017.06.031

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We derive an explicit formula for the intrinsic MacWilliams transform for permutation-invariant qudit codes. Such codes naturally live in symmetric power representations, where the relevant error sectors are determined by the irreducible decomposition of the conjugation action on the associated operator space. Using the multiplicity-free structure of this decomposition and the corresponding intertwiner algebra, we identify the intrinsic MacWilliams matrix with a finite Racah transform. The entries are given by a terminating hypergeometric series, and the rows of the matrix are Racah orthogonal polynomials with parameters determined explicitly by the block length and local dimension. Computing the spectrum of the degree-one twirl reveals that this spectrum lies on an affine quadratic lattice. Then we derive a tridiagonal multiplication rule from the representation theory of the adjoint sector. As consequences, we obtain closed-form orthogonality, detailed-balance, and involutivity identities for the transform. The resulting formula supplies an explicit MacWilliams matrix for computing linear programming bounds on permutation-invariant qudit codes.
We study permutation-invariant quantum codes in the symmetric subspace $\mathrm{Sym}^n(\mathbb{C}^q) $ of nnn qudits of local dimension qqq. For every integer q≥2q\geq 2q≥2, we construct a permutation-invariant code with parameters ((4,q,2))q((4,q,2))_q((4,q,2))q​. Thus four physical qudits suffice to encode one logical qudit with distance two in the symmetric sector for every local dimension. We also show, using linear-programming constraints for permutation-invariant quantum codes, that no permutation-invariant code of dimension qqq and distance at least 222 exists in Symn(Cq)\mathrm{Sym}^n(\mathbb{C}^q)Symn(Cq) for n≤3n\leq 3n≤3. Hence four qudits are necessary and sufficient. The construction has a simple representation-theoretic and combinatorial description. In the irreducible SU(q)\mathrm{SU}(q)SU(q)-module Sym4(Cq)\mathrm{Sym}^4(\mathbb{C}^q)Sym4(Cq), the distance-two Knill-Laflamme conditions split into root and Cartan parts. By restricting supports to the even-entry occupation layer, all root-error conditions vanish automatically. The remaining Cartan conditions reduce to linear balancing constraints on packets of occupation vectors. These packets admit a natural graph-theoretic interpretation in terms of the vertices and edges of the complete graph KqK_qKq​: for odd qqq, they are organized by the midpoint rule, while for even qqq, they are organized by a decomposition of KqK_qKq​ into perfect matchings. In this way, the existence of minimal ((4,q,2))q((4,q,2))_q((4,q,2))q​ permutation-invariant codes is reduced to a parity-dependent edge-coloring problem on KqK_qKq​.
Quantum synchronisation errors are a class of errors that change the number of qubits in a quantum system. The classical error correction of synchronisation errors has been well-studied, including an insertion-deletion equivalence more than a half-century ago, but little progress has been made towards the quantum counterpart since the birth of quantum error correction. We address the longstanding problem of a quantum insertion-deletion equivalence on permutation-invariant codes, detailing the conditions under which such codes are ttt-insertion error-correctable. We extend these conditions to quantum insertion-deletion errors, formulating a more restrictive set of conditions under which permutation-invariant codes are (t,s)(t,s)(t,s)-insdel error-correctable. For completeness, we extend our approach to qudit errors on qudit permutation-invariant codes. Our work resolves many of the outstanding questions regarding the quantum error correction of synchronisation errors.