[Jump to code hierarchy]

2D lattice stabilizer code

Description

Lattice stabilizer code in two Euclidean dimensions.

Any translation-invariant 2D prime-qudit lattice stabilizer code can be converted to several copies of the prime-qudit 2D surface code along with some trivial codes [1]. Any 2D topological order requires weight-four Hamiltonian terms, i.e., it cannot be stabilized via weight-two or weight-three terms on 2D lattices of qubits or qutrits [24].

Translation-invariant 2D prime-qudit lattice stabilizer codes are equivalent to several copies of the prime-qudit surface code and a trivial code via a local constant-depth Clifford circuit [1]. There are algorithms which determine the fusion and braiding rules [5] as well as boundaries and twist defects [6] of a 2D translationally invariant modular-qudit stabilizer code for any qudit dimension.

Encoding

The geometric entanglement measure of a 2D stabilizer codeword with sufficiently high distance \(d\) scales as order \(\Omega(d^2)\) [7].

Decoding

Renormalization group (RG) decoder [8].Tensor-network based decoder for 2D codes subject to correlated noise [9].Standard stabilizer-based error correction can be performed even in the presence of perturbations to the codespace [1012]; see also Refs. [1315].Real-time geometrically local decoder based on introducing an ancillary buffer and confining spacetime interactions between anyons [16].

Code Capacity Threshold

Noise thresholds can be formulated as anyon condensation transitions in a topological field theory [17], generalizing the mapping of the effect of noise on a code state to a statistical mechanical model [9,1820]. Namely, the noise threshold for a noise channel \(\cal{E}\) acting on a 2D stabilizer state \(|\psi\rangle\) can be obtained from the properties of the resulting (mixed) state \(\mathcal{E}(|\psi\rangle\langle\psi|)\) [17,2124].

Cousins

  • Kitaev surface code— Translation-invariant 2D qubit lattice stabilizer codes are equivalent to several copies of the Kitaev surface code via a local constant-depth qudit Clifford circuit [2527].
  • Abelian quantum-double stabilizer code— Translation-invariant 2D prime-qudit lattice stabilizer codes are equivalent to several copies of the prime-qudit surface code and a trivial code via a local constant-depth qudit Clifford circuit [1].
  • Holographic code— 2D lattice stabilizer codes admit a bulk-boundary correspondence similar to that of holographic codes, namely, the boundary Hilbert space of the former cannot be realized via local degrees of freedom [28].
  • Qubit QLDPC code— Chain complexes describing qubit QLDPC codes can be converted to 2D lattice stabilizer codes [29].
  • Self-correcting quantum code— 2D stabilizer codes [30] and encodings of frustration-free code Hamiltonians [31] admit only constant-energy excitations, and so do not have an energy barrier.

Primary Hierarchy

Parents
2D lattice stabilizer code
Children
The Majorana color code is a 2D qubit stabilizer code with respect to the Majorana operator basis.
The Majorana surface code is a 2D qubit stabilizer code with respect to the Majorana operator basis.
The 2D bosonization code encodes fermionic modes into a 2D qubit stabilizer code.
Bivariate bicycle codes are defined on 2D lattices with periodic boundary conditions, and versions with open boundary conditions have been investigated [6,32]. Bivariate bicycle codes are on par with the surface code in terms of threshold, but admit a much higher ancilla-added encoding rate at the expense of having non-geometrically local weight-six check operators. BB codes have been investigated in terms of their anyons and topological order [33].
All Abelian TQD codes can be realized as modular-qudit lattice stabilizer codes by starting with an Abelian quantum double model along with a family of Abelian TQDs that generalize the double semion anyon theory and condensing certain bosonic anyons [34]. Abelian TQD codes need not be translationally invariant and can realize multiple topological phases on one lattice.

References

[1]
J. Haah, “Classification of translation invariant topological Pauli stabilizer codes for prime dimensional qudits on two-dimensional lattices”, Journal of Mathematical Physics 62, (2021) arXiv:1812.11193 DOI
[2]
S. Bravyi and M. Vyalyi, “Commutative version of the k-local Hamiltonian problem and common eigenspace problem”, (2004) arXiv:quant-ph/0308021
[3]
D. Aharonov and L. Eldar, “On the complexity of Commuting Local Hamiltonians, and tight conditions for Topological Order in such systems”, (2011) arXiv:1102.0770
[4]
D. Aharonov, O. Kenneth, and I. Vigdorovich, “On the Complexity of Two Dimensional Commuting Local Hamiltonians”, LIPIcs, Volume 111, TQC 2018 111, 2:1 (2018) arXiv:1803.02213 DOI
[5]
Z. Liang, Y. Xu, J. T. Iosue, and Y.-A. Chen, “Extracting Topological Orders of Generalized Pauli Stabilizer Codes in Two Dimensions”, PRX Quantum 5, (2024) arXiv:2312.11170 DOI
[6]
Z. Liang, B. Yang, J. T. Iosue, and Y.-A. Chen, “Operator algebra and algorithmic construction of boundaries and defects in (2+1)D topological Pauli stabilizer codes”, (2025) arXiv:2410.11942
[7]
Z. Li, D. Lee, and B. Yoshida, “How Much Entanglement Is Needed for Topological Codes and Mixed States with Anomalous Symmetry?”, (2025) arXiv:2405.07970
[8]
G. Duclos-Cianci and D. Poulin, “A renormalization group decoding algorithm for topological quantum codes”, (2010) arXiv:1006.1362
[9]
C. T. Chubb and S. T. Flammia, “Statistical mechanical models for quantum codes with correlated noise”, Annales de l’Institut Henri Poincaré D, Combinatorics, Physics and their Interactions 8, 269 (2021) arXiv:1809.10704 DOI
[10]
E. Lake, S. Balasubramanian, and S. Choi, “Exact Quantum Algorithms for Quantum Phase Recognition: Renormalization Group and Error Correction”, PRX Quantum 6, (2025) arXiv:2211.09803 DOI
[11]
W. Zhong, O. Shtanko, and R. Movassagh, “Advantage of Quantum Neural Networks as Quantum Information Decoders”, (2024) arXiv:2401.06300
[12]
A. Lavasani and S. Vijay, “The Stability of Gapped Quantum Matter and Error-Correction with Adiabatic Noise”, (2024) arXiv:2402.14906
[13]
A. Kay, “Nonequilibrium Reliability of Quantum Memories”, Physical Review Letters 102, (2009) arXiv:0807.0287 DOI
[14]
F. Pastawski, A. Kay, N. Schuch, and I. Cirac, “Limitations of Passive Protection of Quantum Information”, (2009) arXiv:0911.3843
[15]
A. Kay, “Capabilities of a Perturbed Toric Code as a Quantum Memory”, Physical Review Letters 107, (2011) arXiv:1107.3940 DOI
[16]
E. Lake, “Local active error correction from simulated confinement”, (2025) arXiv:2510.08056
[17]
Y. Bao, R. Fan, A. Vishwanath, and E. Altman, “Mixed-state topological order and the errorfield double formulation of decoherence-induced transitions”, (2023) arXiv:2301.05687
[18]
E. Dennis, A. Kitaev, A. Landahl, and J. Preskill, “Topological quantum memory”, Journal of Mathematical Physics 43, 4452 (2002) arXiv:quant-ph/0110143 DOI
[19]
A. A. Kovalev and L. P. Pryadko, “Fault tolerance of quantum low-density parity check codes with sublinear distance scaling”, Physical Review A 87, (2013) arXiv:1208.2317 DOI
[20]
A. A. Kovalev and L. P. Pryadko, “Spin glass reflection of the decoding transition for quantum error correcting codes”, (2014) arXiv:1311.7688
[21]
J. Y. Lee, C.-M. Jian, and C. Xu, “Quantum Criticality Under Decoherence or Weak Measurement”, PRX Quantum 4, (2023) arXiv:2301.05238 DOI
[22]
R. Fan, Y. Bao, E. Altman, and A. Vishwanath, “Diagnostics of Mixed-State Topological Order and Breakdown of Quantum Memory”, PRX Quantum 5, (2024) arXiv:2301.05689 DOI
[23]
Y.-H. Chen and T. Grover, “Separability Transitions in Topological States Induced by Local Decoherence”, Physical Review Letters 132, (2024) arXiv:2309.11879 DOI
[24]
K. Su, Z. Yang, and C.-M. Jian, “Tapestry of dualities in decohered quantum error correction codes”, Physical Review B 110, (2024) arXiv:2401.17359 DOI
[25]
H. Bombin, G. Duclos-Cianci, and D. Poulin, “Universal topological phase of two-dimensional stabilizer codes”, New Journal of Physics 14, 073048 (2012) arXiv:1103.4606 DOI
[26]
H. Bombín, “Structure of 2D Topological Stabilizer Codes”, Communications in Mathematical Physics 327, 387 (2014) arXiv:1107.2707 DOI
[27]
J. Haah, “Algebraic Methods for Quantum Codes on Lattices”, Revista Colombiana de Matemáticas 50, 299 (2017) arXiv:1607.01387 DOI
[28]
T. Schuster, N. Tantivasadakarn, A. Vishwanath, and N. Y. Yao, “A holographic view of topological stabilizer codes”, (2023) arXiv:2312.04617
[29]
X. Li, T.-C. Lin, and M.-H. Hsieh, “Transform Arbitrary Good Quantum LDPC Codes into Good Geometrically Local Codes in Any Dimension”, (2024) arXiv:2408.01769
[30]
S. Bravyi and B. Terhal, “A no-go theorem for a two-dimensional self-correcting quantum memory based on stabilizer codes”, New Journal of Physics 11, 043029 (2009) arXiv:0810.1983 DOI
[31]
O. Landon-Cardinal and D. Poulin, “Local Topological Order Inhibits Thermal Stability in 2D”, Physical Review Letters 110, (2013) arXiv:1209.5750 DOI
[32]
J. N. Eberhardt, F. R. F. Pereira, and V. Steffan, “Pruning qLDPC codes: Towards bivariate bicycle codes with open boundary conditions”, (2024) arXiv:2412.04181
[33]
Anonymous, “Anyon theory and topological frustration of high-efficiency quantum low-density parity-check codes”, Physical Review Letters (2025) arXiv:2503.04699 DOI
[34]
T. D. Ellison, Y.-A. Chen, A. Dua, W. Shirley, N. Tantivasadakarn, and D. J. Williamson, “Pauli Stabilizer Models of Twisted Quantum Doubles”, PRX Quantum 3, (2022) arXiv:2112.11394 DOI
Page edit log

Your contribution is welcome!

on github.com (edit & pull request)— see instructions

edit on this site

Zoo Code ID: 2d_stabilizer

Cite as:
“2D lattice stabilizer code”, The Error Correction Zoo (V. V. Albert & P. Faist, eds.), 2024. https://errorcorrectionzoo.org/c/2d_stabilizer
BibTeX:
@incollection{eczoo_2d_stabilizer, title={2D lattice stabilizer code}, booktitle={The Error Correction Zoo}, year={2024}, editor={Albert, Victor V. and Faist, Philippe}, url={https://errorcorrectionzoo.org/c/2d_stabilizer} }
Share via:
Twitter | Mastodon |  | E-mail
Permanent link:
https://errorcorrectionzoo.org/c/2d_stabilizer

Cite as:

“2D lattice stabilizer code”, The Error Correction Zoo (V. V. Albert & P. Faist, eds.), 2024. https://errorcorrectionzoo.org/c/2d_stabilizer

Github: https://github.com/errorcorrectionzoo/eczoo_data/edit/main/codes/quantum/groups/stabilizer/lattice/2d_stabilizer.yml.