\((2,2)\) Loop toric code[1]
Description
A generalization of the Kitaev surface code defined on a 4D lattice. The code is called a \((2,2)\) toric code because it admits 2D membrane \(Z\)-type and \(X\)-type logical operators. Both types of operators create 1D (i.e., loop) excitations at their edges. The code serves as a self-correcting quantum memory [1,2].
Qubits are placed on plaquettes, each \(Z\)-type stabilizer generator is supported on six plaquettes surrounding an edge, and \(X\)-type stabilizers are placed on the six plaquettes of every cube [3].
Loop toric code often either refers to the construction on the four-dimensional torus or is an alternative name for the general construction.
The construction has been extended to modular qudits [4].
Protection
Code parameters for an open hypercubic lattice of side-length \(L\) are \([[6L^4 − 12L^3 + 10L^2 - 4L + 1, 1, L^2]]\) [5].Encoding
Lindbladian-based dissipative encoding, for which codespace is steady-state space of a Lindbladian [6].Transversal Gates
Only logical Clifford gates can be implemented transversally when defined on a hypercubic lattice [3].Gates
Logical \(S\) gate using physical \(CS\) gates via the Pontryagin square [4].Logical \(CZ\), \(S\), and Hadamard gates when defined on a hypercubic lattice [7].Decoding
Local automaton decoder [8] based on Toom’s rule for the classical 2D repetition code [9–12].Local automaton decoder obtained from reinforcement learning [13].Code Capacity Threshold
Independent \(X,Z\) noise: \(2.117\%\) with Hastings decoder [8] and \(7.3\%\) with RG decoder for 4D surface code [14]. It is conjectured via a statistical-mechanical mapping that the optimal ML decoder yields a threshold of \(11.003\%\) [15].Threshold
Phenomenological noise model for the 4D loop toric code: \(4.35\%\) with RG decoder [14], and \(4.3\%\) under improved BP-OSD decoder [16].Gate-based depolarizing noise: \(0.31\%\) with RG decoder for 4D loop toric code [14].\(1.59\%\) for independent \(X,Z\) noise and faulty syndrome measurements using the Hastings decoder [8].Realizations
Trapped ions: single-shot QEC realized using a \([[33,1,4]]\) rotated version of the loop toric code on the Quantinuum H2 device [5].Cousins
- Higher-dimensional homological product code— The 4D loop planar (toric) code on a hypercubic lattice can be obtained from a particular choice of chain complex from a hypergraph product of four repetition codes [17].
- Repetition code— The 4D loop planar (toric) code on a hypercubic lattice can be obtained from a particular choice of chain complex from a hypergraph product of four repetition codes [17].
- Campbell double homological product code— The 4D loop planar (toric) code on a hypercubic lattice can be obtained from a particular choice of chain complex from a hypergraph product of four repetition codes [17]. As such, it is a particular Campbell double homological product code [18; table I].
- Self-correcting quantum code— For similar reasons as the classical 2D Ising model is a self-correcting classical memory, the 4D loop toric code is a self-correcting quantum memory due to an order \(O(n)\) energy cost of creating a logical error [1,2].
- Haah cubic code (CC)— The energy of any partial implementation of CC1 is proportional to the boundary length similar to the 4D toric code, which can potentially surpress the effects of thermal errors, but it is currently an open problem.
Member of code lists
- Hamiltonian-based codes and friends
- Quantum codes
- Quantum codes based on homological products
- Quantum codes with code capacity thresholds
- Quantum codes with notable decoders
- Quantum codes with other thresholds
- Quantum codes with transversal gates
- Quantum CSS codes
- Quantum LDPC codes
- Realized quantum codes
- Self-correcting quantum codes and friends
- Single-shot codes and friends
- Stabilizer codes
- Surface code and friends
- Topological codes
Primary Hierarchy
References
- [1]
- E. Dennis, A. Kitaev, A. Landahl, and J. Preskill, “Topological quantum memory”, Journal of Mathematical Physics 43, 4452 (2002) arXiv:quant-ph/0110143 DOI
- [2]
- R. Alicki, M. Horodecki, P. Horodecki, and R. Horodecki, “On thermal stability of topological qubit in Kitaev’s 4D model”, (2008) arXiv:0811.0033
- [3]
- T. Jochym-O’Connor and T. J. Yoder, “Four-dimensional toric code with non-Clifford transversal gates”, Physical Review Research 3, (2021) arXiv:2010.02238 DOI
- [4]
- X. Chen, A. Dua, P.-S. Hsin, C.-M. Jian, W. Shirley, and C. Xu, “Loops in 4+1d topological phases”, SciPost Physics 15, (2023) arXiv:2112.02137 DOI
- [5]
- N. Berthusen et al., “Experiments with the four-dimensional surface code on a quantum charge-coupled device quantum computer”, Physical Review A 110, (2024) arXiv:2408.08865 DOI
- [6]
- F. Pastawski, L. Clemente, and J. I. Cirac, “Quantum memories based on engineered dissipation”, Physical Review A 83, (2011) arXiv:1010.2901 DOI
- [7]
- P.-S. Hsin, R. Kobayashi, and G. Zhu, “Non-Abelian Self-Correcting Quantum Memory and Single-shot Non-Clifford Gate beyond the \(n^{1/3}\) Distance Barrier”, (2025) arXiv:2405.11719
- [8]
- N. P. Breuckmann, K. Duivenvoorden, D. Michels, and B. M. Terhal, “Local Decoders for the 2D and 4D Toric Code”, (2016) arXiv:1609.00510
- [9]
- A. L. Toom, “Nonergodic Multidimensional System of Automata”, Probl. Peredachi Inf., 10:3 (1974), 70–79; Problems Inform. Transmission, 10:3 (1974), 239–246
- [10]
- Toom, Andrei L. “Stable and attractive trajectories in multicomponent systems.” Multicomponent random systems 6 (1980): 549-575.
- [11]
- L. F. Gray, “Toom’s Stability Theorem in Continuous Time”, Perplexing Problems in Probability 331 (1999) DOI
- [12]
- G. Grinstein, “Can complex structures be generically stable in a noisy world?”, IBM Journal of Research and Development 48, 5 (2004) DOI
- [13]
- M. Park, N. Maskara, M. Kalinowski, and M. D. Lukin, “Enhancing quantum memory lifetime with measurement-free local error correction and reinforcement learning”, Physical Review A 111, (2025) arXiv:2408.09524 DOI
- [14]
- K. Duivenvoorden, N. P. Breuckmann, and B. M. Terhal, “Renormalization Group Decoder for a Four-Dimensional Toric Code”, IEEE Transactions on Information Theory 65, 2545 (2019) arXiv:1708.09286 DOI
- [15]
- K. Takeda and H. Nishimori, “Self-dual random-plaquette gauge model and the quantum toric code”, Nuclear Physics B 686, 377 (2004) arXiv:hep-th/0310279 DOI
- [16]
- O. Higgott and N. P. Breuckmann, “Improved Single-Shot Decoding of Higher-Dimensional Hypergraph-Product Codes”, PRX Quantum 4, (2023) arXiv:2206.03122 DOI
- [17]
- W. Zeng and L. P. Pryadko, “Higher-Dimensional Quantum Hypergraph-Product Codes with Finite Rates”, Physical Review Letters 122, (2019) arXiv:1810.01519 DOI
- [18]
- E. T. Campbell, “A theory of single-shot error correction for adversarial noise”, Quantum Science and Technology 4, 025006 (2019) arXiv:1805.09271 DOI
Page edit log
- Victor V. Albert (2024-04-26) — most recent
Cite as:
“\((2,2)\) Loop toric code”, The Error Correction Zoo (V. V. Albert & P. Faist, eds.), 2024. https://errorcorrectionzoo.org/c/4d_surface