Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:0710.4271

Asymptotics of the quantum Hamming bound for subsystem codes

Andreas Klappenecker, Pradeep Kiran Sarvepalli

Published Oct 23, 2007• 1 citation
arXivHTMLPDF

Abstract

Ashikhmin and Litsyn showed that all binary stabilizer codes - pure or impure - of sufficiently large length obey the quantum Hamming bound, ruling out the possibility that impure codes of large length can outperform pure codes with respect to sphere packing. In contrast we show that impure subsystem codes do not obey the quantum Hamming bound for pure subsystem codes, not even asymptotically. We show that there exist arbitrarily long Bacon-Shor codes that violate the quantum Hamming bound.

DOI
10.48550/arxiv.0710.4271

Related papers

Progress on Problem about Quantum Hamming Bound for Impure Quantum Codes

Zhuo Li, Lijuan Xing

A famous open problem in the theory of quantum error-correcting codes is whether or not the parameters of an impure quantum code can violate the quantum Hamming bound for pure quantum codes. We partially solve this problem. We demonstrate that there exists a threshold such that an arbitrary quantum code must obey the quantum Hamming bound whenever . We list some values of for small d and binary quantum codes.

arXiv:0907.3802•Jul 22, 2009•0 citations

On subsystem codes beating the quantum Hamming or Singleton bound

Andreas Klappenecker, Pradeep Kiran Sarvepalli

Subsystem codes are a generalization of noiseless subsystems, decoherence-free subspaces and stabilizer codes. We generalize the quantum Singleton bound to q -linear subsystem codes. It follows that no subsystem code over a prime field can beat the quantum Singleton bound. On the other hand, we show the remarkable fact that there exist impure subsystem codes beating the quantum Hamming bound. A number of open problems concern the comparison in the performance of stabilizer and subsystem codes. One of the open problems suggested by Poulin's work asks whether a subsystem code can use fewer syndrome measurements than an optimal q -linear maximum distance separable stabilizer code while encoding the same number of qudits and having the same distance. We prove that linear subsystem codes cannot offer such an improvement under complete decoding.

arXiv:quant-ph/0703213•Proceedings of the Royal Society A Mathematical Physical and Engineering Sciences•Aug 21, 2007•26 citations

On a Problem Concerning the Quantum Hamming Bound for Impure Quantum Codes

Zhuo Li, Lijuan Xing

A famous open problem in the theory of quantum error-correcting codes is whether or not the parameters of an impure quantum code can violate the quantum Hamming bound for pure quantum codes. We partially solve this problem. We demonstrate that there exists a thresholdN(d,m) such that an arbitrary((n,K,d))mquantum code must obey the quantum Hamming bound whenevern≥N(d,m). We list some values ofN(d,m) for smalldand binary quantum codes.

IEEE Transactions on Information Theory•Aug 19, 2010•9 citations

Strengthened quantum Hamming bound

Lijuan Xing, Zhuo Li, Zhang Wu-Jun

By studying sets of operators with constant weight we present for the first time an analytical upper bound on the pure quantum stabilizer codes whose underlying quantum system can be of arbitrary dimension, which outperforms the so far well-known quantum Hamming bound, the optimal analytical upper bound for small code length.

Acta Physica Sinica•Jan 1, 2011•1 citation

The strengthened quantum Hamming bound of Yu, Lai, and Oh

Valery, Grishin, Aryeh Lev Zabokritskiy

We prove a conjecture of Yu, Lai, and Oh: their strengthened quantum Hamming bounds, a family that interpolates between Hamming-type bounds and the Singleton bound, hold for all quantum codes of dimension $K>1$, including impure and nonadditive codes. The result covers every integer local dimension $p\ge2$, not necessarily a prime power, every integer $t\ge1$, both distances $2t+1$ and $2t+2$, and every interpolation parameter $e\in\{0,\ldots,t\}$. The case $e=0$ implies the ordinary quantum Hamming bound for general codes, recently proved by Zhang and Chen. Yu, Lai, and Oh proved their bounds for pure codes and for general codes of distance three or four. More generally, for every integer $p\ge2$ and every quantum code of length $n$, dimension $K>1$ and distance $d\ge3$, we prove $Kf(0)\le p^n\mathbb{E} f(X)$, where $X\sim\operatorname{Bin}(n,1-p^{-2})$, for every real polynomial $f$ of degree less than $d$ that is nonnegative on $\{0,\ldots,n\}$ and positive at zero. For pure codes this inequality is implicit in the argument of Yu, Lai, and Oh. The proof uses the linear-programming method with quantum weight enumerators.

quant-pharXiv:2610.30088•Oct 22, 2026•0 citations

Degeneracy Cannot Violate the Quantum Hamming Bound

Yu-Xuan Zhang, Jing-Ling Chen

The quantum Hamming bound is the standard finite-length sphere-packing bound for exact correction of arbitrary qubit errors. Whether degeneracy can evade this bound has remained unresolved in full generality for nearly three decades: distinct correctable errors may act identically on the code space, so the usual disjoint-sphere argument breaks down. We prove that every exact binary quantum subspace code with $K>1$ obeys the bound, without assuming either nondegeneracy or additivity. Our proof turns the Li--Xing linear-programming polynomial into an exact intersection count for quaternary Hamming balls. Monotonicity in block length and in ball-center separation then reduces the problem to a local node--edge charging inequality at the shortest admissible length. Thus degeneracy can merge correctable error sectors, but cannot enlarge the finite-length binary Hamming bound.

quant-pharXiv:2606.15558•Jun 16, 2026•0 citations
Ashikhmin and Litsyn showed that all binary stabilizer codes - pure or impure - of sufficiently large length obey the quantum Hamming bound, ruling out the possibility that impure codes of large length can outperform pure codes with respect to sphere packing. In contrast we show that impure subsystem codes do not obey the quantum Hamming bound for pure subsystem codes, not even asymptotically. We show that there exist arbitrarily long Bacon-Shor codes that violate the quantum Hamming bound.
Subsystem codes are a generalization of noiseless subsystems, decoherence-free subspaces and stabilizer codes. We generalize the quantum Singleton bound to q -linear subsystem codes. It follows that no subsystem code over a prime field can beat the quantum Singleton bound. On the other hand, we show the remarkable fact that there exist impure subsystem codes beating the quantum Hamming bound. A number of open problems concern the comparison in the performance of stabilizer and subsystem codes. One of the open problems suggested by Poulin's work asks whether a subsystem code can use fewer syndrome measurements than an optimal q -linear maximum distance separable stabilizer code while encoding the same number of qudits and having the same distance. We prove that linear subsystem codes cannot offer such an improvement under complete decoding.
We prove a conjecture of Yu, Lai, and Oh: their strengthened quantum Hamming bounds, a family that interpolates between Hamming-type bounds and the Singleton bound, hold for all quantum codes of dimension K>1K>1K>1, including impure and nonadditive codes. The result covers every integer local dimension p≥2p\ge2p≥2, not necessarily a prime power, every integer t≥1t\ge1t≥1, both distances 2t+12t+12t+1 and 2t+22t+22t+2, and every interpolation parameter e∈{0,…,t}e\in\{0,\ldots,t\}e∈{0,…,t}. The case e=0e=0e=0 implies the ordinary quantum Hamming bound for general codes, recently proved by Zhang and Chen. Yu, Lai, and Oh proved their bounds for pure codes and for general codes of distance three or four. More generally, for every integer p≥2p\ge2p≥2 and every quantum code of length nnn, dimension K>1K>1K>1 and distance d≥3d\ge3d≥3, we prove Kf(0)≤pnEf(X)Kf(0)\le p^n\mathbb{E} f(X)Kf(0)≤pnEf(X), where X∼Bin⁡(n,1−p−2)X\sim\operatorname{Bin}(n,1-p^{-2})X∼Bin(n,1−p−2), for every real polynomial fff of degree less than ddd that is nonnegative on {0,…,n}\{0,\ldots,n\}{0,…,n} and positive at zero. For pure codes this inequality is implicit in the argument of Yu, Lai, and Oh. The proof uses the linear-programming method with quantum weight enumerators.
The quantum Hamming bound is the standard finite-length sphere-packing bound for exact correction of arbitrary qubit errors. Whether degeneracy can evade this bound has remained unresolved in full generality for nearly three decades: distinct correctable errors may act identically on the code space, so the usual disjoint-sphere argument breaks down. We prove that every exact binary quantum subspace code with K>1K>1K>1 obeys the bound, without assuming either nondegeneracy or additivity. Our proof turns the Li--Xing linear-programming polynomial into an exact intersection count for quaternary Hamming balls. Monotonicity in block length and in ball-center separation then reduces the problem to a local node--edge charging inequality at the shortest admissible length. Thus degeneracy can merge correctable error sectors, but cannot enlarge the finite-length binary Hamming bound.