Description
A 3D lattice stabilizer code whose bulk realizes a 3D time-reversal SPT order [1] and whose gapped boundary supports the 2D three-fermion (3F) topological order. The code can be used as a resource state for fault-tolerant MBQC [2].
The code is obtained from two copies of the 3D surface code on a cubic lattice, with qubits \(\sigma\) and \(\tau\) on each edge [1,3]. The vertex terms are those of the two copies. Each face term is decorated by \(\sigma^x\) and \(\tau^x\) operators on the edges lying over and under the face in a fixed 2D projection [3; Eq. (2)]. A string operator of either copy then leaves a line of the other copy’s flux along its length, so point excitations are linearly confined in the bulk [3]. Truncating the stabilizers at a smooth boundary yields deconfined boundary string operators realizing the 3F topological order [1,3].
Encoding
3F QCA encoder [4,5], which can be simplified using bosonization [6] and can be extended to SPTs in higher dimensions based on an exact bosonization duality [7].Gates
Clifford gates can be performed by braiding and fusing symmetry defects in the MBQC model.Fault Tolerance
Fault-tolerant MBQC protocol by encoding in, braiding, and fusing symmetry defects.Cousins
- 3D bosonization code— The 3F Walker-Wang QCA encoder [4,5] can be simplified using bosonization [6].
- Bosonization code— The 3F Walker-Wang QCA encoder [4,5] can be extended to SPTs in higher dimensions based on an exact bosonization duality [7].
- Abelian topological code— The gapped boundary of the 3F Walker-Wang model supports the 3F topological order [1,2].
- 3D surface code— The 3F Walker-Wang model code is obtained from two copies of the 3D surface code on the same cubic lattice [1,3]. The copies are twisted together by decorating the face terms with \(X\)-type operators on the edges lying over and under each face [3]. Flux of one copy then confines the point excitations of the other [3].
- Symmetry-protected self-correcting quantum code— Without symmetry enforcement, the 3F Walker-Wang model code on a \(T^2\times I\) lattice stores no information, even classical, at nonzero temperature [3]. Enforcing the one-form symmetry generated by its vertex terms within a distance \(W\) of one boundary forbids string endpoints there [3]. A boundary logical string must then be completed by bulk strings carrying linearly confined flux, giving a symmetric energy barrier \(\Delta\sim\min\{L_1,L_2,W\}\) on an \(L_1\times L_2\) boundary torus [3]. The two qubits at that boundary thus form a symmetry-protected self-correcting quantum code whenever \(W\), \(L_1\), and \(L_2\) grow without bound [3]. The enforced region can have measure zero in the thermodynamic limit, e.g., for \(W\) growing logarithmically with the lattice size [3].
- Three-fermion (3F) subsystem code— The (three-dimensional) 3F Walker-Wang model cluster-like state encodes the temporal gate operations on the (two-dimensional) 3F subsystem code into a third spatial dimension [2].
- Six-semion stabilizer code— The six-semion and three-fermion anyon theories are the \(r=2\) and \(r=1\) members of the family \(F_{2^r}\) of Abelian anyon theories with fusion group \(\mathbb{Z}_{2^r}\times\mathbb{Z}_{2^r}\) [8,9].
Primary Hierarchy
References
- [1]
F. J. Burnell, X. Chen, L. Fidkowski, and A. Vishwanath, “Exactly soluble model of a three-dimensional symmetry-protected topological phase of bosons with surface topological order”, Physical Review B 90, (2014) arXiv:1302.7072 DOI
- [2]
S. Roberts and D. J. Williamson, “3-Fermion Topological Quantum Computation”, PRX Quantum 5, (2024) arXiv:2011.04693 DOI
- [3]
C. Stahl and R. Nandkishore, “Symmetry-protected self-correcting quantum memory in three space dimensions”, Physical Review B 103, (2021) arXiv:2103.08622 DOI
- [4]
J. Haah, L. Fidkowski, and M. B. Hastings, “Nontrivial Quantum Cellular Automata in Higher Dimensions”, Communications in Mathematical Physics 398, 469 (2022) arXiv:1812.01625 DOI
- [5]
J. Haah, “Topological Phases of Unitary Dynamics: Classification in Clifford Category”, Communications in Mathematical Physics 406, (2025) arXiv:2205.09141 DOI
- [6]
L. Fidkowski and M. B. Hastings, “Pumping Chirality in Three Dimensions”, (2024) arXiv:2309.15903
- [7]
L. Fidkowski, J. Haah, and M. B. Hastings, “A quantum cellular automaton for every symmetry protected topological phase”, Physical Review B 112, (2025) arXiv:2407.07951 DOI
- [8]
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
- [9]
L. Wang and Z. Wang, “In and around abelian anyon models \({}^{
* }\)”, Journal of Physics A: Mathematical and Theoretical 53, 505203 (2020) DOI
Page edit log
- Victor V. Albert (2026-11-06) — most recent
- Victor V. Albert (2026-10-26)
- Victor V. Albert (2026-06-08)
- Victor V. Albert (2023-03-28)
Cite as:
“Three-fermion (3F) Walker-Wang model code”, The Error Correction Zoo (V. V. Albert & P. Faist, eds.), 2026. https://errorcorrectionzoo.org/c/three_fermion, arXiv:2606.11484