pith. machine review for the scientific record. sign in

arxiv: 2604.22521 · v2 · submitted 2026-04-24 · 🪐 quant-ph · cond-mat.stat-mech· cond-mat.str-el

Recognition: unknown

Decohered color code and emerging mixed toric code by anyon proliferation: Topological entanglement negativity perspective

Authors on Pith no claims yet

Pith reviewed 2026-05-08 11:48 UTC · model grok-4.3

classification 🪐 quant-ph cond-mat.stat-mechcond-mat.str-el
keywords color codetoric codedecoherencemixed-state topological ordertopological entanglement negativityanyon proliferationstabilizer states
0
0 comments X

The pith

Decoherence via XX operators on red links turns the color code into a mixed state that inherits half its topological properties and emerges as a single toric code.

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

The paper investigates decoherence effects on the color code defined on a honeycomb lattice. It demonstrates that XX-type decoherence on red links produces a mixed state retaining half the topological features of the pure color code, including anyon content and logical operators. This leads to an intrinsic mixed-state topological order identified as related to a toric code through a gauging procedure. Topological entanglement negativity serves as the key diagnostic, decreasing from 2 ln 2 to ln 2 at maximum decoherence. Simulations show a smooth crossover with a variance peak, and scaling behavior specific to certain subsystem partitions.

Core claim

For decoherence induced by XX-type operators on red links of the honeycomb lattice, the resulting mixed state inherits half of the topological properties of the color code, including anyon content, logical operators, and topological entanglement structure. Using a gauging procedure for mixed stabilizer states, the emergent phase is identified as closely related to a single toric code. The pure color code has TEN = 2 ln 2, while the maximally decohered state has TEN = ln 2, indicating emergence of a single toric code. Tuning the decoherence strength reveals a smooth crossover in TEN with a pronounced peak in its variance.

What carries the argument

Topological entanglement negativity (TEN) as a probe combined with gauging of mixed stabilizer states to identify the emergent toric code phase.

If this is right

  • The decohered mixed state possesses the anyon content and logical operators of a single toric code.
  • TEN exhibits a smooth crossover with a nearly system-size-independent peak in variance as decoherence strength varies.
  • The negativity shows characteristic scaling only for subsystem partitions matching the triangular lattice of the emergent toric code.
  • Negativity-based quantities can probe mixed-state topological order generated by decoherence.

Where Pith is reading between the lines

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

  • Decoherence channels could be engineered to create other mixed topological phases from known codes.
  • The variance peak in TEN might signal a transition point between different mixed phases.
  • Similar anyon proliferation effects may occur in other quantum error correcting codes under targeted noise.

Load-bearing premise

The gauging procedure for mixed stabilizer states correctly identifies the emergent phase as a single toric code without missing additional effects from the decoherence channel.

What would settle it

A direct computation or measurement of the anyon content or logical operators in the maximally decohered state that fails to match those expected for a toric code.

Figures

Figures reproduced from arXiv: 2604.22521 by Ikuo Ichinose, Keisuke Kataoka, Takahiro Orito, Yoshihito Kuno.

Figure 1
Figure 1. Figure 1: FIG. 1. Schematic image of color code system. (a) Image of the lattice and the definitions of plaquette site, vertex and length of the system view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. The color-code system for the analytical calculation of the view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. The color-code system for the analytical calculation of the view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Subsystem complex used for calculation of the TEN. Bound view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. Setting of the subsystems for the calculation of view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. (Upper panel) The value of TEN, view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9. (a) Calculations of view at source ↗
read the original abstract

We study how the color code under decoherence gives rise to an intrinsic mixed-state topological order (imTO), which has no counterpart in pure ground states of local gapped Hamiltonians. For decoherence induced by XX-type operators on red links of the honeycomb lattice, we show that the resulting mixed state inherits half of the topological properties of the color code, including anyon content, logical operators, and topological entanglement structure. Using a gauging procedure for mixed stabilizer states, we identify the emergent phase as closely related to a single toric code. We characterize this phase by topological entanglement negativity (TEN) and perform efficient stabilizer-formalism simulations. While the pure color code has ${\rm TEN} = 2 \ln 2$, the maximally decohered state has ${\rm TEN} = \ln 2$, indicating emergence of a single toric code. By tuning the decoherence strength, we find a smooth crossover in TEN accompanied by a pronounced, nearly system-size-independent peak in its variance. We further show that the negativity exhibits characteristic scaling only for subsystem partitions commensurate with the triangular lattice of the emergent toric code. Our results demonstrate that negativity-based quantities provide powerful probes of mixed-state topological order generated by decoherence.

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

0 major / 3 minor

Summary. The manuscript studies decoherence of the color code on the honeycomb lattice via XX-type operators acting on red links. It claims that the resulting mixed state exhibits an intrinsic mixed-state topological order (imTO) that inherits half the topological properties of the pure color code, including anyon content, logical operators, and entanglement structure. A gauging procedure for mixed stabilizer states is used to identify the emergent phase as closely related to a single toric code. Topological entanglement negativity (TEN) is computed via stabilizer simulations, yielding TEN = 2 ln 2 for the pure color code and TEN = ln 2 for the maximally decohered state; a smooth crossover with a nearly system-size-independent variance peak is reported, together with partition-dependent scaling of the negativity.

Significance. If the central claims hold, the work advances the understanding of decoherence-induced intrinsic mixed-state topological order, which lacks a pure-state counterpart. Strengths include the exact TEN values (2 ln 2 to ln 2), the use of efficient stabilizer-formalism simulations to obtain concrete numerical results, the system-size-independent variance peak, and the demonstration that negativity scaling appears only for partitions commensurate with the emergent toric-code lattice. These provide falsifiable, negativity-based diagnostics for anyon proliferation in mixed topological phases and have implications for topological quantum error correction under decoherence.

minor comments (3)
  1. [Gauging procedure] The gauging procedure for mixed stabilizer states is load-bearing for the phase identification; the main text should include an explicit step-by-step construction (or a clear reference to prior work) showing how the anyon content is halved and how the logical operators are inherited, including any assumptions on the decoherence channel.
  2. [Numerical results] The abstract and results section report a 'nearly system-size-independent' variance peak in TEN; please add the specific system sizes simulated, the number of samples, error bars or statistical uncertainties, and the precise criterion used to identify the peak location.
  3. [Topological entanglement negativity] The claim that negativity exhibits characteristic scaling 'only for subsystem partitions commensurate with the triangular lattice' would benefit from an explicit definition of the partitions used and a brief discussion of why incommensurate partitions fail to show the scaling.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive assessment of our manuscript and the recommendation for minor revision. The referee's summary accurately captures our central results on decoherence-induced intrinsic mixed-state topological order in the color code, the emergence of a single toric code, and the use of topological entanglement negativity as a diagnostic. We appreciate the recognition of the strengths, including the exact TEN values, stabilizer simulations, system-size-independent variance peak, and partition-dependent scaling. As no specific major comments were raised in the report, we will incorporate minor improvements in the revised version.

Circularity Check

0 steps flagged

No significant circularity; derivation relies on direct stabilizer simulations and independent gauging

full rationale

The paper's central results follow from explicit stabilizer-formalism simulations of the XX-decohered color code on the honeycomb lattice, followed by a gauging map applied to the resulting mixed stabilizer state and direct computation of topological entanglement negativity (TEN) for chosen partitions. The reduction from pure color code TEN = 2 ln 2 to maximal-decoherence TEN = ln 2 is obtained by evaluating the negativity formula on the decohered density matrix; it is not obtained by fitting a parameter or by renaming an input. The gauging procedure is invoked as a standard tool for mixed stabilizer states rather than a self-citation whose validity depends on the present work. No self-definitional loop, fitted-input-as-prediction, or ansatz-smuggled-via-citation appears in the derivation chain. The lattice-partition dependence of the negativity scaling is likewise a direct numerical observation, not a tautology.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The central claim rests on the standard definition of the color code, the validity of the mixed-state gauging map, and the interpretation of TEN as a faithful probe of mixed topological order.

free parameters (1)
  • decoherence strength
    Tuned continuously to observe the smooth crossover and variance peak in TEN.
axioms (2)
  • domain assumption The color code on the honeycomb lattice supports the stated anyon content and logical operators.
    Standard background for topological stabilizer codes.
  • domain assumption Topological entanglement negativity correctly diagnoses the inherited topological order in the mixed state.
    Central diagnostic used throughout the work.

pith-pipeline@v0.9.0 · 5546 in / 1521 out tokens · 39472 ms · 2026-05-08T11:48:52.451329+00:00 · methodology

discussion (0)

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

Reference graph

Works this paper leans on

95 extracted references · 14 canonical work pages · 1 internal anchor

  1. [1]

    This allows us to quotient the deconfined anyon set by fusion withrX, leading to an emergent toric-code-type modular structure

    AlthoughrXis not literally absorbed into the vacuum sector in the gauge-out description [40], it acts as a transparent anyon that is invisible to all braiding pro- cesses involving the surviving deconfined excitations. This allows us to quotient the deconfined anyon set by fusion withrX, leading to an emergent toric-code-type modular structure. In this se...

  2. [2]

    transition

    In the present system, therXanyon behaves in a manner analogous to anyon condensation [42, 55]. However, it is not absorbed into the vacuum sector and instead re- mains as a transparent anyon. Consequently, the result- ing structure is more appropriately understood not as a true anyon condensation, but as a modular quotient of a non-modular theory arising...

  3. [3]

    7-plaquette

    conjectured that the negativityN A also satisfies a scaling law such as NA =c|∂A| −γ N +· · ·,(28) wherecis a non-universal constant and|∂A|is the perimeter of the subsystem A. (As explained later, this length unit is altered depending on the relevant degree of freedom of states.) On the other hand,γ N is the TEN, which can be a universal quantity in the ...

  4. [4]

    subsection, we observed some peculiar behavior of the TEN and its variance

    The number of samples isO(10 3). subsection, we observed some peculiar behavior of the TEN and its variance. We wonder if large fluctuations in the TEN come from those of the ingredient negativity or the manipu- lation to obtain the TEN by combining the negativity of the subsystems. Following numerical study clarifies both of the above issues. In Fig. 8, ...

  5. [5]

    Obtained numerical data of⟨N A⟩obviously support this scaling law

    It is also expected that for the TC limit,N A =|∂A| TC −1 = 1 2 (|∂A| −2)suggesting this normalization. Obtained numerical data of⟨N A⟩obviously support this scaling law. (b) Sample-to-sample variance ofN A divided by (|∂Ai| −2). VI. CONCLUSION AND DISCUSSION In this work, we studied the color code under the deco- herence of theXXtype acting on red edges ...

  6. [6]

    Wen, Rev

    X.-G. Wen, Rev. Mod. Phys.89, 041004 (2017)

  7. [7]

    B. Zeng, X. Chen, D.-L. Zhou, and X.-G. Wen, Quantum information meets quantum matter – from quantum entan- glement to topological phase in many-body systems (2018), arXiv:1508.02595 [cond-mat.str-el]

  8. [8]

    Nayak, S

    C. Nayak, S. H. Simon, A. Stern, M. Freedman, and S. Das Sarma, Rev. Mod. Phys.80, 1083 (2008)

  9. [9]

    A. Y . Kitaev, Russian Mathematical Surveys52, 1191 (1997)

  10. [10]

    Kitaev, Annals of Physics303, 2–30 (2003)

    A. Kitaev, Annals of Physics303, 2–30 (2003)

  11. [11]

    The Heisenberg Representation of Quantum Computers

    D. Gottesman, The heisenberg representation of quantum com- puters (1998), arXiv:quant-ph/9807006 [quant-ph]

  12. [12]

    B. M. Terhal, Rev. Mod. Phys.87, 307 (2015)

  13. [13]

    Fujii, Quantum computation with topological codes: from qubit to topological fault-tolerance (2015), arXiv:1504.01444 [quant-ph]

    K. Fujii, Quantum computation with topological codes: from qubit to topological fault-tolerance (2015), arXiv:1504.01444 [quant-ph]

  14. [14]

    Dennis, A

    E. Dennis, A. Kitaev, A. Landahl, and J. Preskill, Journal of Mathematical Physics43, 4452–4505 (2002)

  15. [15]

    Arakawa and I

    G. Arakawa and I. Ichinose, Annals of Physics311, 152 (2004)

  16. [16]

    T. Ohno, G. Arakawa, I. Ichinose, and T. Matsui, Nuclear Physics B697, 462 (2004)

  17. [17]

    Fujii and Y

    K. Fujii and Y . Tokunaga, Phys. Rev. A86, 020303 (2012)

  18. [18]

    K. G. Wilson, Phys. Rev. D10, 2445 (1974)

  19. [19]

    ’t Hooft, Nuclear Physics B138, 1 (1978)

    G. ’t Hooft, Nuclear Physics B138, 1 (1978)

  20. [20]

    Kitaev and J

    A. Kitaev and J. Preskill, Phys. Rev. Lett.96, 110404 (2006)

  21. [21]

    Bombin and M

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

  22. [22]

    Bombin, R

    H. Bombin, R. S. Andrist, M. Ohzeki, H. G. Katzgraber, and M. A. Martin-Delgado, Phys. Rev. X2, 021004 (2012)

  23. [23]

    Lidar and T

    D. Lidar and T. Brun, Quantum Error Correction (Cambridge University Press, 2013)

  24. [24]

    Bomb ´ın, New Journal of Physics17, 083002 (2015)

    H. Bomb ´ın, New Journal of Physics17, 083002 (2015)

  25. [25]

    Bombin, G

    H. Bombin, G. Duclos-Cianci, and D. Poulin, New Journal of Physics14, 073048 (2012)

  26. [26]

    Lavasani, Y

    A. Lavasani, Y . Alavirad, and M. Barkeshli, Phys. Rev. Lett. 127, 235701 (2021)

  27. [27]

    G.-Y . Zhu, N. Tantivasadakarn, and S. Trebst, Phys. Rev. Res. 6, L042063 (2024)

  28. [28]

    Sriram, T

    A. Sriram, T. Rakovszky, V . Khemani, and M. Ippoliti, Phys. Rev. B108, 094304 (2023)

  29. [29]

    Y . Kuno, T. Orito, and I. Ichinose, Phys. Rev. B109, 054432 (2024)

  30. [30]

    Orito, Y

    T. Orito, Y . Kuno, and I. Ichinose, Phys. Rev. B109, 224306 (2024)

  31. [31]

    Botzung, M

    T. Botzung, M. Buchhold, S. Diehl, and M. M ¨uller, Journal of Physics A: Mathematical and Theoretical58, 205304 (2025)

  32. [32]

    Kataoka, Y

    K. Kataoka, Y . Kuno, T. Orito, and I. Ichinose, Phys. Rev. B 113, 024111 (2026)

  33. [33]

    Raussendorf and H

    R. Raussendorf and H. J. Briegel, Phys. Rev. Lett.86, 5188 (2001)

  34. [34]

    Raussendorf, D

    R. Raussendorf, D. E. Browne, and H. J. Briegel, Phys. Rev. A 68, 022312 (2003)

  35. [35]

    H. J. Briegel, D. E. Browne, W. D ¨ur, R. Raussendorf, and M. Van den Nest, Nature Physics5, 19 (2009)

  36. [36]

    Efficiently preparing GHZ, topologi- cal and fracton states by measuring cold atoms

    R. Verresen, N. Tantivasadakarn, and A. Vishwanath, Effi- ciently preparing schr ¨odinger’s cat, fractons and non-abelian topological order in quantum devices (2022), arXiv:2112.03061 [quant-ph]

  37. [37]

    T.-C. Lu, Z. Zhang, S. Vijay, and T. H. Hsieh, PRX Quantum4, 030318 (2023)

  38. [38]

    Tantivasadakarn, R

    N. Tantivasadakarn, R. Thorngren, A. Vishwanath, and R. Ver- resen, Phys. Rev. X14, 021040 (2024)

  39. [39]

    Y . Kuno, T. Orito, and I. Ichinose, Phys. Rev. B110, 014110 (2024)

  40. [40]

    M. A. Nielsen and I. L. Chuang, Quantum Computation and Quantum Information, 10th ed. (Cambridge University Press, USA, 2011)

  41. [41]

    R. Fan, Y . Bao, E. Altman, and A. Vishwanath, PRX Quantum 5, 020343 (2024)

  42. [42]

    S. Sang, Y . Zou, and T. H. Hsieh, Phys. Rev. X14, 031044 (2024)

  43. [43]

    Negari, T

    A.-R. Negari, T. D. Ellison, and T. H. Hsieh, Spacetime markov length: a diagnostic for fault tolerance via mixed-state phases (2025), arXiv:2412.00193 [quant-ph]

  44. [44]

    Z. Wang, Z. Wu, and Z. Wang, PRX Quantum6, 010314 (2025)

  45. [45]

    Sohal and A

    R. Sohal and A. Prem, PRX Quantum6, 010313 (2025)

  46. [46]

    Sang and T

    S. Sang and T. H. Hsieh, Phys. Rev. Lett.134, 070403 (2025)

  47. [47]

    T. D. Ellison and M. Cheng, PRX Quantum6, 010315 (2025)

  48. [48]

    Y . Kuno, T. Orito, and I. Ichinose, Phys. Rev. B111, 064111 (2025)

  49. [49]

    P.-S. Hsin, R. Kobayashi, and A. Prem, Higher-form anomalies imply intrinsic long-range entanglement (2025), arXiv:2504.10569 [quant-ph]

  50. [50]

    Levin and X.-G

    M. Levin and X.-G. Wen, Phys. Rev. Lett.96, 110405 (2006)

  51. [51]

    R. F. Werner, Phys. Rev. A40, 4277 (1989)

  52. [52]

    Groisman, S

    B. Groisman, S. Popescu, and A. Winter, Phys. Rev. A72, 032317 (2005)

  53. [53]

    Horodecki, P

    R. Horodecki, P. Horodecki, M. Horodecki, and K. Horodecki, Rev. Mod. Phys.81, 865 (2009). 18

  54. [54]

    Peres, Phys

    A. Peres, Phys. Rev. Lett.77, 1413 (1996)

  55. [55]

    Vidal and R

    G. Vidal and R. F. Werner, Phys. Rev. A65, 032314 (2002)

  56. [56]

    M. B. Plenio, Phys. Rev. Lett.95, 090503 (2005)

  57. [57]

    R. Fan, Y . Bao, E. Altman, and A. Vishwanath, PRX Quantum 5, 10.1103/prxquantum.5.020343 (2024)

  58. [58]

    Kubica, B

    A. Kubica, B. Yoshida, and F. Pastawski, New Journal of Physics17, 083026 (2015)

  59. [59]

    A. B. Aloshious and P. K. Sarvepalli, Phys. Rev. A100, 012348 (2019)

  60. [60]

    M. S. Kesselring, J. C. Magdalena de la Fuente, F. Thomsen, J. Eisert, S. D. Bartlett, and B. J. Brown, PRX Quantum5, 010342 (2024)

  61. [61]

    Cai and M

    K.-L. Cai and M. Cheng, Entanglement negativity in decohered topological states (2026), arXiv:2602.16597 [cond-mat.str-el]

  62. [62]

    Aaronson and D

    S. Aaronson and D. Gottesman, Phys. Rev. A70, 052328 (2004)

  63. [63]

    T. D. Ellison, Y .-A. Chen, A. Dua, W. Shirley, N. Tanti- vasadakarn, and D. J. Williamson, Quantum7, 1137 (2023)

  64. [64]

    Yoshida, Phys

    B. Yoshida, Phys. Rev. B91, 245131 (2015)

  65. [65]

    Nussinov and G

    Z. Nussinov and G. Ortiz, Proceedings of the Na- tional Academy of Sciences106, 16944 (2009), https://www.pnas.org/doi/pdf/10.1073/pnas.0803726105

  66. [66]

    Nussinov and G

    Z. Nussinov and G. Ortiz, Annals of Physics324, 977 (2009)

  67. [67]

    Gaiotto, A

    D. Gaiotto, A. Kapustin, N. Seiberg, and B. Willett, Journal of High Energy Physics2015, 10.1007/jhep02(2015)172 (2015)

  68. [68]

    McGreevy, Annual Review of Condensed Matter Physics14, 57–82 (2023)

    J. McGreevy, Annual Review of Condensed Matter Physics14, 57–82 (2023)

  69. [69]

    Weinstein, Y

    Z. Weinstein, Y . Bao, and E. Altman, Phys. Rev. Lett.129, 080501 (2022)

  70. [70]

    Kargarian, H

    M. Kargarian, H. Bombin, and M. A. Martin-Delgado, New Journal of Physics12, 025018 (2010)

  71. [71]

    M. R. Haghighi and M. H. Zarei, Phys. Rev. B112, 165126 (2025)

  72. [72]

    Bu ˇca and T

    B. Bu ˇca and T. Prosen, New J. of Phys.14, 073007 (2012)

  73. [73]

    V . V . Albert and L. Jiang, Phys. Rev. A89, 022118 (2014)

  74. [74]

    de Groot, A

    C. de Groot, A. Turzillo, and N. Schuch, Quantum6, 856 (2022)

  75. [75]

    S. Sang, Y . Li, T. Zhou, X. Chen, T. H. Hsieh, and M. P. Fisher, PRX Quantum2, 030313 (2021)

  76. [76]

    T.-C. Lu, T. H. Hsieh, and T. Grover, Phys. Rev. Lett.125, 116801 (2020)

  77. [77]

    Anzai, H

    K. Anzai, H. Matsueda, and Y . Kuno, Phys. Rev. B113, 014111 (2026)

  78. [78]

    B. Shi, X. Dai, and Y .-M. Lu, Entanglement negativity at the critical point of measurement-driven transition (2021), arXiv:2012.00040 [cond-mat.stat-mech]

  79. [79]

    Sharma, X

    S. Sharma, X. Turkeshi, R. Fazio, and M. Dalmonte, SciPost Phys. Core5, 023 (2022)

  80. [80]

    Y . Kuno, T. Orito, and I. Ichinose, Phys. Rev. B108, 094104 (2023)

Showing first 80 references.