pith. sign in

arxiv: 2605.15266 · v1 · submitted 2026-05-14 · 🪐 quant-ph · cs.ET

Synthesis and Optimization of Encoding Circuits for Fault-Tolerant Quantum Computation

Pith reviewed 2026-05-19 16:19 UTC · model grok-4.3

classification 🪐 quant-ph cs.ET
keywords stabilizer codesencoder synthesisfault-tolerant quantum computationquantum circuit optimizationholographic codesquantum LDPC codesstabilizer tableau
0
0 comments X p. Extension

The pith

Search over stabilizer tableaus yields encoders for arbitrary stabilizer codes with up to 43% fewer two-qubit gates.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper sets out to show that efficient circuits for preparing arbitrary logical states in stabilizer codes can be found by treating encoder synthesis as a search over stabilizer tableaus. It introduces greedy and rollout-based algorithms that exploit the existence of multiple stabilizer-equivalent realizations of the same encoding isometry to reduce gate count and depth. For codes with modular structure the approach builds large encoders from locally optimized pieces obtained via exact SMT synthesis. When applied to families including holographic and qLDPC codes the resulting circuits use fewer resources than prior constructions, lowering the cost of state preparation in fault-tolerant schemes.

Core claim

By searching among stabilizer-equivalent tableaus the authors obtain encoding circuits for arbitrary stabilizer codes whose two-qubit gate counts and depths are lower than those of existing constructions, with the improvement arising directly from the systematic use of the freedom among equivalent realizations.

What carries the argument

Search over stabilizer tableaus navigated by greedy and rollout algorithms that identify low-cost stabilizer-equivalent realizations of the encoding isometry.

If this is right

  • Lower gate counts reduce the physical resource overhead of state preparation in any fault-tolerant scheme that relies on encoded logical states.
  • Reduced circuit depth limits error accumulation during the preparation step itself.
  • Modular composition from exact local solutions makes synthesis tractable for structured code families at larger scales.
  • The same search formulation can be reused for other isometry synthesis tasks that admit stabilizer-tableau descriptions.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The tableau-search technique might transfer to optimizing other stabilizer-circuit primitives such as logical measurements or syndrome extraction.
  • For codes lacking obvious modular structure, hybrid methods that seed the search with known good subcircuits could further improve scaling.
  • Widespread adoption would shift the bottleneck in fault-tolerant resource estimation from encoder construction to other overhead sources such as magic-state distillation.

Load-bearing premise

The greedy and rollout search algorithms will reliably locate high-quality stabilizer-equivalent realizations without becoming trapped in poor local optima for the codes of practical interest.

What would settle it

A concrete calculation that produces an encoder for a specific stabilizer code whose two-qubit gate count exceeds that of a known hand-optimized construction from the literature would show the search methods do not always reach the claimed savings.

Figures

Figures reproduced from arXiv: 2605.15266 by Matthew Steinberg, Robert Wille, Sascha Heu{\ss}en, Tom Peham.

Figure 1
Figure 1. Figure 1: FIG. 1: A ZX diagram representation of the [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: Encoding circuit synthesis as state space search. Every state corresponds to an intermediate circuit and [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: A ZX diagram representation of the [PITH_FULL_IMAGE:figures/full_fig_p010_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: Encoding circuit synthesis of the [PITH_FULL_IMAGE:figures/full_fig_p011_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5 [PITH_FULL_IMAGE:figures/full_fig_p012_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6: ZX-diagram of a holographic HaPPY [ [PITH_FULL_IMAGE:figures/full_fig_p013_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7: Encoding circuits for the 12-qubit HaPPY code obtained from two modular synthesis strategies. [PITH_FULL_IMAGE:figures/full_fig_p018_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8: Impact of early termination on encoding circuits with rollout level [PITH_FULL_IMAGE:figures/full_fig_p030_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9: Impact of early termination on encoding circuits with rollout level [PITH_FULL_IMAGE:figures/full_fig_p031_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: FIG. 10: Impact of early termination on encoding circuits with rollout level [PITH_FULL_IMAGE:figures/full_fig_p032_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: FIG. 11: Impact of early termination on encoding circuits with rollout level [PITH_FULL_IMAGE:figures/full_fig_p033_11.png] view at source ↗
read the original abstract

Preparing arbitrary logical states is a central primitive for universal fault-tolerant quantum computation and the cost of encoded-state preparation contributes directly to the overall resource overhead. This makes the synthesis of efficient general-state encoding circuits an important problem, particularly with respect to two-qubit gate count and circuit depth. Yet the synthesis of such encoders has been studied less extensively than general Clifford circuit synthesis or the preparation of specific logical Pauli-eigenstates. In this work, we develop methods for synthesizing efficient encoders for arbitrary stabilizer codes. We formulate encoder synthesis as a search over stabilizer tableaus and introduce greedy and rollout-based algorithms that exploit the freedom among stabilizer-equivalent realizations of the same encoding isometry. For code families with a modular structure, such as generalized concatenated and holographic codes, we show how large encoders can be assembled from optimized local constituent encoders, and we use SMT-based exact synthesis to obtain optimal local circuits for small instances. We further evaluate the proposed methods on a broad set of stabilizer codes, including holographic and quantum low-density parity-check (qLDPC) codes, and compare them against recent encoder-synthesis methods and existing constructions from the literature, obtaining improvements of up to 43% in two-qubit gate count and up to 70% in depth. Our results support the optimization of encoded-state preparation in several fault-tolerant quantum-computing schemes, and all methods are openly available as part of the Munich Quantum Toolkit.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript develops methods for synthesizing efficient encoders for arbitrary stabilizer codes by formulating the problem as a search over stabilizer tableaus. It introduces greedy and rollout-based algorithms that exploit stabilizer-equivalent realizations of the encoding isometry, assembles large encoders from optimized local constituents for modular codes (e.g., generalized concatenated and holographic) using SMT-based exact synthesis for small instances, and reports empirical evaluations on a broad set of codes including qLDPC and holographic families. The work claims concrete improvements of up to 43% in two-qubit gate count and 70% in depth relative to recent synthesis methods and literature constructions, with all methods released in the Munich Quantum Toolkit.

Significance. If the empirical gains are reproducible and the heuristics scale reliably, the results would reduce overhead for general logical-state preparation, a key primitive in fault-tolerant schemes. The open-source release and evaluation across diverse code families (including practically relevant qLDPC) are strengths that support adoption. The approach fills a gap between general Clifford synthesis and preparation of specific eigenstates.

major comments (2)
  1. [§4.1–4.2] §4.1–4.2 (greedy and rollout algorithms): These are local heuristics without optimality guarantees or escape mechanisms from poor local optima. The central claim of up to 43% gate-count and 70% depth improvements for arbitrary stabilizer codes rests on reliable discovery of high-quality realizations; for larger instances the tableau search space grows rapidly, yet no analysis of entrapment frequency, multiple random restarts, or scaling behavior is provided. This is load-bearing for the generality of the reported gains.
  2. [§5] §5 (evaluation and comparisons): The reported percentage improvements are measured against external literature constructions, but the manuscript does not detail the exact baseline circuits, whether identical optimization targets (gate count vs. depth) were used, or statistical controls such as number of heuristic trials. Without these, it is difficult to verify that the gains are representative rather than instance-specific.
minor comments (2)
  1. [§2.2] §2.2 (tableau notation): An explicit small-code example mapping a stabilizer tableau to the corresponding encoding circuit would improve accessibility for readers outside the immediate subfield.
  2. [Figure 5] Figure 5 (assembled encoder diagrams): Labeling the boundaries of the SMT-optimized local subcircuits would clarify how the modular construction contributes to the overall depth reduction.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive feedback on our manuscript. We address the major comments point by point below and have revised the manuscript to incorporate clarifications and additional analysis where feasible.

read point-by-point responses
  1. Referee: [§4.1–4.2] §4.1–4.2 (greedy and rollout algorithms): These are local heuristics without optimality guarantees or escape mechanisms from poor local optima. The central claim of up to 43% gate-count and 70% depth improvements for arbitrary stabilizer codes rests on reliable discovery of high-quality realizations; for larger instances the tableau search space grows rapidly, yet no analysis of entrapment frequency, multiple random restarts, or scaling behavior is provided. This is load-bearing for the generality of the reported gains.

    Authors: We agree that the greedy and rollout algorithms are local heuristics without formal optimality guarantees. In the revised manuscript we have added an explicit discussion of the multiple random restarts already present in our implementation, together with new empirical measurements of entrapment frequency and runtime scaling on larger tableau instances (now included in Section 4 and Appendix C). These data show that the reported improvements remain stable across restarts for the evaluated code families, although we acknowledge that exhaustive optimality proofs for arbitrary codes remain out of reach. revision: partial

  2. Referee: [§5] §5 (evaluation and comparisons): The reported percentage improvements are measured against external literature constructions, but the manuscript does not detail the exact baseline circuits, whether identical optimization targets (gate count vs. depth) were used, or statistical controls such as number of heuristic trials. Without these, it is difficult to verify that the gains are representative rather than instance-specific.

    Authors: We accept this observation. The revised Section 5 now lists the precise literature circuits used as baselines, states that separate optimizations were performed for gate count and for depth, and reports the number of heuristic trials (100 restarts per instance) together with mean and standard-deviation statistics. These additions allow direct verification of the reported gains. revision: yes

Circularity Check

0 steps flagged

No significant circularity; algorithmic synthesis with external benchmarks

full rationale

The paper formulates encoder synthesis as a search over stabilizer tableaus and introduces greedy/rollout algorithms plus SMT exact synthesis for small modular components. Reported gains (up to 43% gate count, 70% depth) are obtained by direct comparison of the synthesized circuits against prior constructions in the literature on concrete code families including qLDPC and holographic codes. No equation, prediction, or central claim reduces by construction to a fitted parameter, self-defined quantity, or load-bearing self-citation; the derivation chain consists of independent algorithmic steps whose outputs are validated externally.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The work rests on the standard stabilizer formalism and the existence of equivalent tableau representations of the same encoding isometry; no new free parameters or invented physical entities are introduced.

axioms (1)
  • standard math Stabilizer formalism and tableau representation of Clifford operations and encoding isometries
    Invoked throughout to define the search space of equivalent encoders.

pith-pipeline@v0.9.0 · 5789 in / 1107 out tokens · 40806 ms · 2026-05-19T16:19:09.963107+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

92 extracted references · 92 canonical work pages · 5 internal anchors

  1. [1]

    Wille, et al., in2024 IEEE International Conference on Quantum Software (QSW)(IEEE, 2024) pp

    R. Wille, et al., in2024 IEEE International Conference on Quantum Software (QSW)(IEEE, 2024) pp. 1–8

  2. [2]

    D. A. Lidar and T. A. Brun,Quantum error correction (Cambridge University Press, 2013)

  3. [3]

    S. J. Devitt, W. J. Munro, and K. Nemoto,Quantum er- ror correction for beginners, Rep. Prog. Phys.76, 076001 (2013)

  4. [4]

    Google Quantum AI,Quantum error correction below the surface code threshold, Nature638, 920–926 (2024)

  5. [5]

    Pogorelov, et al.,Experimental fault-tolerant code switching, Nat

    I. Pogorelov, et al.,Experimental fault-tolerant code switching, Nat. Phys.21, 298–303 (2025)

  6. [6]

    C. Ryan-Anderson, et al.,High-fidelity and Fault-tolerant Teleportation of a Logical Qubit using Transversal Gates and Lattice Surgery on a Trapped-ion Quantum Com- puter(2024), arXiv:2404.16728 [quant-ph]

  7. [7]

    Bluvstein, et al.,Logical quantum processor based on reconfigurable atom arrays, Nature626, 58–65 (2024)

    D. Bluvstein, et al.,Logical quantum processor based on reconfigurable atom arrays, Nature626, 58–65 (2024)

  8. [8]

    Bravyi and A

    S. Bravyi and A. Kitaev,Universal quantum computation with ideal Clifford gates and noisy ancillas, Phys. Rev. A 71, 022316 (2005)

  9. [9]

    M. E. Beverland, A. Kubica, and K. M. Svore,Cost of Universality: A Comparative Study of the Overhead of State Distillation and Code Switching with Color Codes, PRX Quantum2, 020341 (2021)

  10. [10]

    P. S. Rodriguez, et al.,Experimental demonstration of logical magic state distillation(2024), arXiv:2412.15165 [quant-ph]

  11. [11]

    Chamberland and A

    C. Chamberland and A. W. Cross,Fault-tolerant magic state preparation with flag qubits, Quantum3, 143 (2019)

  12. [12]

    Magic state cultivation: growing T states as cheap as CNOT gates

    C. Gidney, N. Shutty, and C. Jones,Magic state cultiva- tion: growing T states as cheap as CNOT gates(2024), arXiv:2409.17595 [quant-ph]

  13. [13]

    Sahay, et al.,Fold-transversal surface code cultivation (2026), arXiv:2509.05212 [quant-ph]

    K. Sahay, et al.,Fold-transversal surface code cultivation (2026), arXiv:2509.05212 [quant-ph]

  14. [14]

    E. Tham, M. Ye, I. Khait, J. Gamble, and N. Delfosse, Distributed fault-tolerant quantum memories over a 2xL array of qubit modules(2025), arXiv:2508.01879 [quant- ph]

  15. [15]

    Clayton and B

    C. Clayton and B. Avritzer,Distributed Quantum Er- ror Correction with Permutation-Invariant Approximate Codes(2025), arXiv:2509.25093 [quant-ph]

  16. [16]

    Gottesman,Surviving as a Quantum Computer in a Classical World(2026), draft textbook manuscript

    D. Gottesman,Surviving as a Quantum Computer in a Classical World(2026), draft textbook manuscript

  17. [17]

    Gidney,Stim: a fast stabilizer circuit simulator, Quan- tum5, 497 (2021)

    C. Gidney,Stim: a fast stabilizer circuit simulator, Quan- tum5, 497 (2021)

  18. [18]

    J. Z. Lu, A. B. Khesin, and P. W. Shor,Uni- versal graph representation of stabilizer codes(2024), arXiv:2411.14448 [quant-ph]

  19. [19]

    Webster, S

    M. Webster, S. Koutsioumpas, and D. E. Browne,Heuris- tic and Optimal Synthesis of CNOT and Clifford Circuits (2025), arXiv:2503.14660 [quant-ph]

  20. [20]

    Peham, N

    T. Peham, N. Brandl, R. Kueng, R. Wille, and L. Burgholzer, in2023 IEEE Int. Conf. Quantum Com- put. Eng. (QCE), Vol. 01 (2023) pp. 802–813

  21. [21]

    Bravyi, J

    S. Bravyi, J. A. Latone, and D. Maslov,6-qubit optimal Clifford circuits, npj Quantum Inf.8, 1–12 (2022)

  22. [22]

    Bravyi, R

    S. Bravyi, R. Shaydulin, S. Hu, and D. Maslov,Clifford Circuit Optimization with Templates and Symbolic Pauli Gates, Quantum5, 580 (2021)

  23. [23]

    K. N. Patel, I. L. Markov, and J. P. Hayes,Optimal syn- thesis of linear reversible circuits, Quantum Info. Com- put.8, 282–294 (2008)

  24. [24]

    Yamasaki and M

    H. Yamasaki and M. Koashi,Time-efficient constant- space-overhead fault-tolerant quantum computation, Nat. Phys.20, 247–253 (2024)

  25. [25]

    Yoshida, S

    S. Yoshida, S. Tamiya, and H. Yamasaki,Concatenate codes, save qubits, npj Quantum Inf.11, 88 (2025)

  26. [26]

    Concatenated Quantum Codes

    E. Knill and R. Laflamme,Concatenated quantum codes (1996), arXiv:quant-ph/9608012 [quant-ph]

  27. [27]

    Fan, et al.,LEGO HQEC: Automating the Analy- sis, Construction, and Decoding of Holographic Quantum Codes(2024), arXiv:2410.22861 [quant-ph]

    J. Fan, et al.,LEGO HQEC: Automating the Analy- sis, Construction, and Decoding of Holographic Quantum Codes(2024), arXiv:2410.22861 [quant-ph]

  28. [28]

    Jahn and J

    A. Jahn and J. Eisert,Holographic tensor network models and quantum error correction: a topical review, Quantum Sci. Technol.6, 033002 (2021)

  29. [29]

    Pastawski, B

    F. Pastawski, B. Yoshida, D. Harlow, and J. Preskill, Holographic quantum error-correcting codes: Toy mod- els for the bulk/boundary correspondence, J. High Energy Phys.2015(6), 1–55

  30. [30]

    R. J. Harris, N. A. McMahon, G. K. Brennen, and T. M. Stace,Calderbank-Shor-Steane holographic quan- tum error-correcting codes, Phys. Rev. A98, 052301 (2018)

  31. [31]

    R. J. Harris, E. Coupe, N. A. McMahon, G. K. Brennen, and T. M. Stace,Decoding holographic codes with an in- teger optimization decoder, Phys. Rev. A102, 062417 (2020)

  32. [32]

    Steinberg, et al.,Far from perfect: Quantum error correction with (hyperinvariant) evenbly codes, Quantum 9, 1826 (2025)

    M. Steinberg, et al.,Far from perfect: Quantum error correction with (hyperinvariant) evenbly codes, Quantum 9, 1826 (2025)

  33. [33]

    Steinberg, et al.,Universal fault-tolerant logic with heterogeneous holographic codes(2025), arXiv:2504.10386 [quant-ph]

    M. Steinberg, et al.,Universal fault-tolerant logic with heterogeneous holographic codes(2025), arXiv:2504.10386 [quant-ph]

  34. [34]

    Goubault de Brugi` ere, S

    T. Goubault de Brugi` ere, S. Martiel, and C. Vuillot,A graph-state based synthesis framework for Clifford isome- tries, Quantum9, 1589 (2025)

  35. [35]

    Kanomata and H

    N. Kanomata and H. Goto,Fault-tolerant quantum com- puting with a high-rate symplectic double code(2025), arXiv:2509.15457 [quant-ph]

  36. [36]

    Bravyi, et al.,High-threshold and low-overhead fault- tolerant quantum memory, Nature627, 778–782 (2024)

    S. Bravyi, et al.,High-threshold and low-overhead fault- tolerant quantum memory, Nature627, 778–782 (2024)

  37. [37]

    Aaronson and D

    S. Aaronson and D. Gottesman,Improved simulation of stabilizer circuits, Phys. Rev. A70, 052328 (2004)

  38. [38]

    van de Wetering,ZX-calculus for the working quantum computer scientist(2020), arXiv:2012.13966 [quant-ph]

    J. van de Wetering,ZX-calculus for the working quantum computer scientist(2020), arXiv:2012.13966 [quant-ph]

  39. [39]

    Kissinger and J

    A. Kissinger and J. van de Wetering,Reducing the num- ber of non-Clifford gates in quantum circuits, Phys. Rev. A102, 022406 (2020)

  40. [40]

    J. Riu, J. Nogu´ e, G. Vilaplana, A. Garcia-Saez, and M. P. Estarellas,Reinforcement Learning Based Quan- tum Circuit Optimization via ZX-Calculus, Quantum9, 1758 (2025)

  41. [41]

    Villoria, H

    A. Villoria, H. Basold, and A. Laarman,Optimisation and synthesis of quantum circuits with global gates, Quan- tum Sci. Technol.11, 015040 (2026)

  42. [42]

    Kissinger,Phase-free ZX diagrams are CSS codes (...or how to graphically grok the surface code)(2022), arXiv:2204.14038 [quant-ph]

    A. Kissinger,Phase-free ZX diagrams are CSS codes (...or how to graphically grok the surface code)(2022), arXiv:2204.14038 [quant-ph]

  43. [43]

    K. H. Wan, H. C. W. Price, and Q. Yao,Holographic codes seen through ZX-calculus(2026), arXiv:2601.04467 [quant-ph]. 21

  44. [44]

    Rodatz, B

    B. Rodatz, B. Po´ or, and A. Kissinger,Fault Tolerance by Construction(2025), arXiv:2506.17181 [quant-ph]

  45. [45]

    Townsend-Teague, J

    A. Townsend-Teague, J. Magdalena de la Fuente, and M. Kesselring,Floquetifying the Colour Code, Electron. Proc. Theor. Comput. Sci.384, 265–303 (2023)

  46. [46]

    Jiang, et al., inProc

    J. Jiang, et al., inProc. 31st ACM-SIAM Symp. Discrete Algorithms (SODA)(SIAM, 2020) pp. 213–229

  47. [47]

    Peham, L

    T. Peham, L. Schmid, L. Berent, M. M¨ uller, and R. Wille, Automated Synthesis of Fault-Tolerant State Prepara- tion Circuits for Quantum Error-Correction Codes, PRX Quantum6, 020330 (2025)

  48. [48]

    Zen, et al.,Quantum Circuit Discovery for Fault- Tolerant Logical State Preparation with Reinforcement Learning, Phys

    R. Zen, et al.,Quantum Circuit Discovery for Fault- Tolerant Logical State Preparation with Reinforcement Learning, Phys. Rev. X15, 041012 (2025)

  49. [49]

    Angl` es Munn´ e, V

    G. Angl` es Munn´ e, V. Kasper, and F. Huber,Engineering holography with stabilizer graph codes, npj Quantum Inf. 10, 48 (2024)

  50. [50]

    Pllaha, K

    T. Pllaha, K. Volanto, and O. Tirkkonen, in2021 IEEE Glob. Commun. Conf. (GLOBECOM)(2021) pp. 01–06

  51. [51]

    A. R. Calderbank and P. W. Shor,Good quantum error- correcting codes exist, Phys. Rev. A54, 1098–1105 (1996)

  52. [52]

    Multiple Particle Interference and Quantum Error Correction

    A. Steane,Multiple Particle Interference and Quantum Error Correction, Proc. R. Soc. Lond. A452, 2551–2577 (1996), arXiv:quant-ph/9601029

  53. [53]

    P. W. Shor, inProc. 37th Conf. Found. Comput. Sci. (IEEE Comput. Soc. Press, Burlington, VT, USA, 1996) pp. 56–65

  54. [54]

    A. M. Steane,Error Correcting Codes in Quantum The- ory, Phys. Rev. Lett.77, 793–797 (1996)

  55. [55]

    P. E. Hart, N. J. Nilsson, and B. Raphael,A Formal Basis for the Heuristic Determination of Minimum Cost Paths, IEEE Trans. Syst. Sci. Cybern.4, 100–107 (1968)

  56. [56]

    D. P. Bertsekas, J. N. Tsitsiklis, and C. Wu,Rollout Al- gorithms for Combinatorial Optimization, J. Heuristics 3, 245–262 (1997)

  57. [57]

    Grassl, P

    M. Grassl, P. Shor, G. Smith, J. Smolin, and B. Zeng, Generalized concatenated quantum codes, Phys. Rev. A 79, 050306 (2009)

  58. [58]

    J. Fan, M. Steinberg, A. Jahn, C. Cao, and S. Feld,Biased-Noise Thresholds of Zero-Rate Holo- graphic Codes with Tensor-Network Decoding, arXiv preprint arXiv:2408.06232 (2024)

  59. [59]

    Z. Wu, S. Cheng, and B. Zeng,A ZX-calculus ap- proach for the construction of graph codes(2024), arXiv:2304.08363 [quant-ph]

  60. [60]

    Steinberg, S

    M. Steinberg, S. Feld, and A. Jahn,Holographic codes from hyperinvariant tensor networks, Nat. Commun.14, 7314 (2023)

  61. [61]

    Gottesman,Stabilizer Codes and Quantum Error Cor- rection, Ph.D

    D. Gottesman,Stabilizer Codes and Quantum Error Cor- rection, Ph.D. thesis, California Institute of Technology (1997)

  62. [62]

    Cabello, L

    A. Cabello, L. E. Danielsen, A. J. L´ opez-Tarrida, and J. R. Portillo,Optimal preparation of graph states, Phys. Rev. A83, 042314 (2011)

  63. [63]

    de Moura and N

    L. de Moura and N. Bjørner, inTools and Algorithms for the Construction and Analysis of Systems, edited by C. R. Ramakrishnan and J. Rehof (Springer Berlin Hei- delberg, Berlin, Heidelberg, 2008) pp. 337–340

  64. [64]

    Duncan and M

    R. Duncan and M. Lucas,Verifying the Steane code with Quantomatic, Electron. Proc. Theor. Comput. Sci.171, 33–49 (2014)

  65. [65]

    Cao and B

    C. Cao and B. Lackey,Quantum Lego: Building Quan- tum Error Correction Codes from Tensor Networks, PRX Quantum3, 020332 (2022)

  66. [66]

    Pastawski and J

    F. Pastawski and J. Preskill,Code properties from holo- graphic geometries, Phys. Rev. X7, 021022 (2017)

  67. [67]

    Almheiri, X

    A. Almheiri, X. Dong, and D. Harlow,Bulk locality and quantum error correction in AdS/CFT, J. High Energy Phys.2015(4), 1–34

  68. [68]

    C. Cao, M. J. Gullans, B. Lackey, and Z. Wang,Quantum lego expansion pack: Enumerators from tensor networks, PRX Quantum5, 030313 (2024)

  69. [69]

    Bombin and M

    H. Bombin and M. A. Martin-Delgado,Topological Quan- tum Distillation, Phys. Rev. Lett.97, 180501 (2006)

  70. [70]

    Bombin and M

    H. Bombin and M. A. Martin-Delgado,Exact topologi- cal quantum order inD= 3and beyond: Branyons and brane-net condensates, Phys. Rev. B75, 075103 (2007)

  71. [71]

    A. M. Steane,Simple quantum error-correcting codes, Phys. Rev. A54, 4741–4751 (1996)

  72. [72]

    Gottesman,Class of quantum error-correcting codes saturating the quantum Hamming bound, Phys

    D. Gottesman,Class of quantum error-correcting codes saturating the quantum Hamming bound, Phys. Rev. A 54, 1862–1868 (1996)

  73. [73]

    Fault-tolerant ancilla preparation and noise threshold lower bounds for the 23-qubit Golay code

    A. Paetznick and B. W. Reichardt,Fault-tolerant ancilla preparation and noise threshold lower bounds for the 23- qubit Golay code(2013), arXiv:1106.2190 [quant-ph]

  74. [74]

    Backens, H

    M. Backens, H. Miller-Bakewell, G. de Felice, L. Lobski, and J. van de Wetering,There and back again: A circuit extraction tale, Quantum5, 421 (2021)

  75. [75]

    Duncan, A

    R. Duncan, A. Kissinger, S. Perdrix, and J. van de Weter- ing,Graph-theoretic Simplification of Quantum Circuits with the ZX-calculus, Quantum4, 279 (2020)

  76. [76]

    Goto,Minimizing resource overheads for fault-tolerant preparation of encoded states of the Steane code, Sci

    H. Goto,Minimizing resource overheads for fault-tolerant preparation of encoded states of the Steane code, Sci. Rep. 6, 19578 (2016)

  77. [77]

    Postler, et al.,Demonstration of fault-tolerant univer- sal quantum gate operations, Nature605, 675 (2022)

    L. Postler, et al.,Demonstration of fault-tolerant univer- sal quantum gate operations, Nature605, 675 (2022)

  78. [78]

    Dasu, et al.,Breaking even with magic: demonstra- tion of a high-fidelity logical non-Clifford gate(2025), arXiv:2506.14688 [quant-ph]

    S. Dasu, et al.,Breaking even with magic: demonstra- tion of a high-fidelity logical non-Clifford gate(2025), arXiv:2506.14688 [quant-ph]

  79. [79]

    J. P. Bonilla Ataides, et al.,Constant-Overhead Fault- Tolerant Bell-Pair Distillation Using High-Rate Codes, Phys. Rev. Lett.135, 130804 (2025)

  80. [80]

    Belzig and H

    P. Belzig and H. Yamasaki,Constant-space-overhead fault-tolerant quantum input/output and communication (2026), arXiv:2602.09103 [quant-ph]

Showing first 80 references.