# Honeycomb Floquet code[1]

## Description

Floquet code based on the Kitaev honeycomb model [2] whose logical qubits are generated through a particular sequence of measurements. A CSS version of the code has been proposed which loosens the restriction of which sequences to use [3]. The code has also been generalized to arbitrary non-chiral, Abelian topological order [4].

The code is defined on a hexagonal (honeycomb) lattice with a physical qubit located at each vertex. Edges are labeled \(x\), \(y\), and \(z\), such that one edge of each label meet at every vertex. Check operators are defined as \(XX\) acting on any two qubits joined by an \(x\) edge, and similarly for \(y\) and \(z\). The hexagonal lattice is 3-colorable, so the hexagons may be labeled 0, 1, 2 such that no two neighboring hexagons have the same label.

The code-generating measurement pattern consists of measuring the check operators located on all of the \(r\)-labeled edges in round \(r\) mod 3. The code space is the \(+1\) eigenspace of the instantaneous stabilizer group (ISG). The ISG specifies the state of the system as a Pauli stabilizer state at a particular round of measurement, and it evolves into a (potentially) different ISG depending on the check operators measured.

## Protection

## Encoding

## Gates

## Decoding

## Fault Tolerance

## Threshold

## Realizations

## Parent

- Hastings-Haah Floquet code — The honeycomb Floquet code is the first 2D Floquet code.

## Cousins

- \(\mathbb{Z}_q^{(1)}\) subsystem code — The dynamically generated logical qubit of the honeycomb Floquet code is generated by appropriately scheduling measurements of the gauge generators of the \(\mathbb{Z}_{q=2}^{(1)}\) subsystem stabilizer code corresponding to the Kitaev honeycomb model. However, since this subsystem code has zero logical qubits, the instantaneous stabilizer codes of the honeycomb code cannot be interpreted as gauge-fixed versions of this subsystem code.
- Kitaev surface code — Measurement of each check operator of the honeycomb Floquet code involves two qubits and projects the state of the two qubits to a two-dimensional subspace, which we regard as an effective qubit. These effective qubits form a surface code on a hexagonal superlattice. Electric and magnetic operators on the embedded surface code correspond to outer logical operators of the Floquet code. In fact, outer logical operators transition back and forth from magnetic to electric surface code operators under the measurement dynamics. Inspired by the honeycomb Floquet code, various weight-two measurement schemes have been designed [17–19], with the scheme in Ref. [18] being a special case of DWR. Numerical comparisons have been performed [20].
- Twist-defect surface code — Fermionic string excitations of the honeycomb Floquet code can be condensed along one-dimensional paths, yielding twist defects [8].
- Subsystem color code — Both honeycomb and subsystem color codes are generated via periodic sequences of measurements. However, any measurement sequence can be performed on the color code without destroying the logical qubits, while honeycomb codes can be maintained only with specific sequences. Honeycomb codes require a shorter measurement cycle and use fewer qubits at the given code distance [1].
- Majorana stabilizer code — The Honeycomb code admits a convenient representation in terms of Majorana fermions. This leads to a possible physical realization of the code in terms of tetrons [21], where each physical qubit is composed of four Majorana modes.
- Quantum LDPC (QLDPC) code — The Floquet check operators are weight-two, and each qubit participates in one check each round.
- Kitaev honeycomb code — The Kitaev honeycomb model Hamiltonian is a sum of checks of the honeycomb Floquet code [1].
- \(A_2\) hexagonal lattice code — The honeycomb Floquet code is defined on the honeycomb lattice.
- Projective-plane surface code — Implementing the honeycomb Floquet code on a non-orientable cross-cap geometry allows for a logical-\(HZ\) gate to be implemented via a measurement schedule [22].

## References

- [1]
- M. B. Hastings and J. Haah, “Dynamically Generated Logical Qubits”, Quantum 5, 564 (2021) arXiv:2107.02194 DOI
- [2]
- A. Kitaev, “Anyons in an exactly solved model and beyond”, Annals of Physics 321, 2 (2006) arXiv:cond-mat/0506438 DOI
- [3]
- M. Davydova, N. Tantivasadakarn, and S. Balasubramanian, “Floquet Codes without Parent Subsystem Codes”, PRX Quantum 4, (2023) arXiv:2210.02468 DOI
- [4]
- J. Sullivan, R. Wen, and A. C. Potter, “Floquet codes and phases in twist-defect networks”, (2023) arXiv:2303.17664
- [5]
- J. Haah and M. B. Hastings, “Boundaries for the Honeycomb Code”, Quantum 6, 693 (2022) arXiv:2110.09545 DOI
- [6]
- C. Vuillot, “Planar Floquet Codes”, (2021) arXiv:2110.05348
- [7]
- D. Aasen, Z. Wang, and M. B. Hastings, “Adiabatic paths of Hamiltonians, symmetries of topological order, and automorphism codes”, Physical Review B 106, (2022) arXiv:2203.11137 DOI
- [8]
- T. D. Ellison, J. Sullivan, and A. Dua, “Floquet codes with a twist”, (2023) arXiv:2306.08027
- [9]
- C. Cesare et al., “Adiabatic topological quantum computing”, Physical Review A 92, (2015) arXiv:1406.2690 DOI
- [10]
- Y.-C. Zheng and T. A. Brun, “Fault-tolerant holonomic quantum computation in surface codes”, Physical Review A 91, (2015) arXiv:1411.4248 DOI
- [11]
- P. Zanardi and M. Rasetti, “Holonomic quantum computation”, Physics Letters A 264, 94 (1999) arXiv:quant-ph/9904011 DOI
- [12]
- D. Gottesman and L. L. Zhang, “Fibre bundle framework for unitary quantum fault tolerance”, (2017) arXiv:1309.7062
- [13]
- C. Gidney et al., “A Fault-Tolerant Honeycomb Memory”, Quantum 5, 605 (2021) arXiv:2108.10457 DOI
- [14]
- C. Gidney, M. Newman, and M. McEwen, “Benchmarking the Planar Honeycomb Code”, Quantum 6, 813 (2022) arXiv:2202.11845 DOI
- [15]
- A. Paetznick et al., “Performance of Planar Floquet Codes with Majorana-Based Qubits”, PRX Quantum 4, (2023) arXiv:2202.11829 DOI
- [16]
- Wootton, James R., “Quantum error correction: From the blackboard to the cloud”, University of Basel (2023) arXiv:2210.13154 DOI
- [17]
- R. Chao et al., “Optimization of the surface code design for Majorana-based qubits”, Quantum 4, 352 (2020) arXiv:2007.00307 DOI
- [18]
- C. Gidney, “A Pair Measurement Surface Code on Pentagons”, Quantum 7, 1156 (2023) arXiv:2206.12780 DOI
- [19]
- L. Grans-Samuelsson et al., “Improved Pairwise Measurement-Based Surface Code”, Quantum 8, 1429 (2024) arXiv:2310.12981 DOI
- [20]
- P. Hilaire et al., “Enhanced Fault-tolerance in Photonic Quantum Computing: Floquet Code Outperforms Surface Code in Tailored Architecture”, (2024) arXiv:2410.07065
- [21]
- T. Karzig et al., “Scalable designs for quasiparticle-poisoning-protected topological quantum computation with Majorana zero modes”, Physical Review B 95, (2017) arXiv:1610.05289 DOI
- [22]
- R. Kobayashi and G. Zhu, “Cross-Cap Defects and Fault-Tolerant Logical Gates in the Surface Code and the Honeycomb Floquet Code”, PRX Quantum 5, (2024) arXiv:2310.06917 DOI

## Page edit log

- Victor V. Albert (2022-06-28) — most recent
- Victor V. Albert (2022-03-02)
- Chris Fechisin (2021-12-13)

## Cite as:

“Honeycomb Floquet code”, The Error Correction Zoo (V. V. Albert & P. Faist, eds.), 2022. https://errorcorrectionzoo.org/c/honeycomb