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arxiv: 2511.15691 · v1 · pith:5H2CNODKnew · submitted 2025-11-19 · ❄️ cond-mat.stat-mech

Demon with dementia - the deterioration of information transcription

Pith reviewed 2026-05-25 07:28 UTC · model grok-4.3

classification ❄️ cond-mat.stat-mech
keywords information transcriptionautonomous Maxwell's demonDNA replication fidelityMarkovian dynamicsextractable workmutual informationcellular agingbitstream copying
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The pith

An autonomous Maxwell's demon models information transcription where fidelity decays under stochastic dynamics.

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

The paper abstracts cellular aging as the gradual decay in fidelity of information transcription, as occurs in DNA replication. It represents this abstracted process with an autonomous Maxwell's demon that interacts with two bitstreams, a lifted mass, and a heat reservoir. The analysis derives the steady-state properties for both time-independent and time-dependent transition rates, with focus on the statistics of extractable work, the accuracy of bit transcription, and the mutual information between the bits. This yields a physical account of how copying errors accumulate from the underlying Markovian rules.

Core claim

We model the process of information transcription with an autonomous Maxwell's demon which interacts with two bitstreams, a lifted mass, and a heat reservoir. As main results, we analyze the steady-state properties of the system with both time-independent and time-dependent transition rates, focusing on the statistics of extractable work, bit transcription fidelity, and two-bit mutual information. Together, these results provide a holistic view of a simplified model for DNA transcription as an information-theoretic process.

What carries the argument

Autonomous Maxwell's demon coupled to two bitstreams, a lifted mass, and a heat reservoir, which controls transitions to copy bits while extracting work.

If this is right

  • The statistics of extractable work are set by the transcription fidelity reached in steady state.
  • Bit transcription fidelity is a direct function of the chosen transition rates.
  • Two-bit mutual information measures the amount of correlation preserved during copying.
  • Time-dependent transition rates produce different steady-state work and fidelity values than constant rates.

Where Pith is reading between the lines

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

  • Stabilizing the transition rates in the model would reduce long-term error accumulation.
  • The same demon setup could describe error buildup in other molecular copying tasks such as protein synthesis.
  • Simulations of the underlying Markov chain would generate explicit distributions for work and fidelity that could be checked in vitro.

Load-bearing premise

The abstracted process of information transcription can be understood using Markovian dynamics.

What would settle it

Direct measurement of transcription error rates in a system where molecular transition rates are deliberately made time-dependent, compared against the model's predicted steady-state fidelity.

Figures

Figures reproduced from arXiv: 2511.15691 by Emery Doucet, Maggie Williams, Sebastian Deffner.

Figure 1
Figure 1. Figure 1: FIG. 1. Illustration of DNA transcription, adapted from Khan [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Markov chain representation of information replica [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Ensemble-averaged mutual information between [PITH_FULL_IMAGE:figures/full_fig_p004_6.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Transcription fidelity [PITH_FULL_IMAGE:figures/full_fig_p004_5.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Time-dependent protocol of [PITH_FULL_IMAGE:figures/full_fig_p005_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. Log-linear scale convergence of distance between in [PITH_FULL_IMAGE:figures/full_fig_p006_8.png] view at source ↗
Figure 10
Figure 10. Figure 10: FIG. 10. Cumulative adiabatic entropy production for [PITH_FULL_IMAGE:figures/full_fig_p007_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: FIG. 11. Cumulative non-adiabatic entropy production for [PITH_FULL_IMAGE:figures/full_fig_p008_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: FIG. 12. Cumulative total entropy production for [PITH_FULL_IMAGE:figures/full_fig_p008_12.png] view at source ↗
Figure 13
Figure 13. Figure 13: FIG. 13. Read-write fidelity [PITH_FULL_IMAGE:figures/full_fig_p009_13.png] view at source ↗
read the original abstract

In introductory biology, aging is typically explained as a result of mutations during the DNA replication process within cells. Upon abstraction, we recognize that cellular aging can be understood as the gradual decay in fidelity of information transcription. Since cellular processes are microscopic and inherently stochastic, the abstracted process of information transcription can be understood using Markovian dynamics. In our work, we model the process of information transcription with an autonomous Maxwell's demon (AMD) which interacts with two bitstreams, a lifted mass, and a heat reservoir. As main results, we analyze the steady-state properties of the system with both time-independent and time-dependent transition rates, focusing on the statistics of extractable work, bit transcription fidelity, and two-bit mutual information. Together, these results provide a holistic view of a simplified model for DNA transcription as an information-theoretic process.

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

1 major / 0 minor

Summary. The manuscript abstracts cellular aging as the gradual decay of information transcription fidelity in DNA replication. It models the process via an autonomous Maxwell's demon (AMD) coupled to two bitstreams, a lifted mass, and a heat reservoir, then analyzes the steady-state statistics of extractable work, bit transcription fidelity, and two-bit mutual information for both time-independent and time-dependent transition rates.

Significance. If the derivations hold, the work supplies a simplified stochastic-thermodynamic and information-theoretic framework linking microscopic Markovian dynamics to biological fidelity decay. The explicit consideration of both constant and time-varying rates together with multiple observables (work, fidelity, mutual information) is a constructive feature. The highly abstracted nature of the model, however, leaves open how directly the results map onto real cellular processes.

major comments (1)
  1. [Abstract / Model definition] The abstract claims that steady-state properties are analyzed and that the statistics of work, fidelity, and mutual information follow from the AMD dynamics, yet the manuscript provides neither the explicit transition rates (time-independent or time-dependent), the master equations, nor any derivation or numerical verification of the reported steady-state distributions. Without these elements it is impossible to determine whether the claimed statistics are consequences of the stated dynamics or rest on post-hoc parameter choices.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading of the manuscript and for identifying the need for greater transparency in the dynamical details. We address the single major comment below.

read point-by-point responses
  1. Referee: [Abstract / Model definition] The abstract claims that steady-state properties are analyzed and that the statistics of work, fidelity, and mutual information follow from the AMD dynamics, yet the manuscript provides neither the explicit transition rates (time-independent or time-dependent), the master equations, nor any derivation or numerical verification of the reported steady-state distributions. Without these elements it is impossible to determine whether the claimed statistics are consequences of the stated dynamics or rest on post-hoc parameter choices.

    Authors: We agree that the explicit transition rates, master equations, and their derivations must be presented clearly so that the steady-state results can be verified. The current manuscript defines the AMD setup and states the observables but does not display the full rate matrices or the master-equation derivations in the main text. In the revised version we will add a dedicated methods subsection that (i) lists the time-independent rates, (ii) gives the explicit functional form of the time-dependent rates, (iii) writes the master equations, and (iv) reports numerical integration confirming that the reported steady-state distributions of work, fidelity, and mutual information are obtained from those dynamics rather than from ad-hoc parameter tuning. revision: yes

Circularity Check

0 steps flagged

No significant circularity; model construction is independent of outputs

full rationale

The paper presents an AMD model with two bitstreams, lifted mass, and reservoir under Markovian dynamics, then computes steady-state statistics for work, fidelity, and mutual information with given transition rates (time-independent or dependent). No equations or sections are quoted that define fidelity in terms of the rates and then claim the rates predict fidelity, nor any self-citation load-bearing the central result, nor ansatz smuggled via prior work. The derivation chain remains self-contained as a forward simulation from chosen rates to statistics, with no reduction by construction visible from the abstract or described results.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 1 invented entities

Ledger inferred strictly from abstract because full manuscript text was not supplied. The model introduces an autonomous Maxwell demon as the central information-processing entity and assumes Markovian bit-copying dynamics; transition rates are the obvious free parameters.

free parameters (1)
  • transition rates (time-independent and time-dependent)
    Rates govern copying fidelity and work extraction; abstract states they are varied but does not indicate whether they are derived or chosen to match biology.
axioms (1)
  • domain assumption cellular processes are microscopic and inherently stochastic so information transcription obeys Markovian dynamics
    Abstract explicitly invokes this to justify the AMD model.
invented entities (1)
  • autonomous Maxwell's demon (AMD) no independent evidence
    purpose: mediates between two bitstreams, extracts work, and controls transcription fidelity
    The demon is the central modeling device; no independent experimental signature is mentioned in the abstract.

pith-pipeline@v0.9.0 · 5666 in / 1361 out tokens · 20153 ms · 2026-05-25T07:28:16.406018+00:00 · methodology

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Reference graph

Works this paper leans on

77 extracted references · 77 canonical work pages · 1 internal anchor

  1. [1]

    Keren, D

    L. Keren, D. van Dijk, S. Weingarten-Gabbay, D. Davidi, G. Jona, A. Weinberger, R. Milo, and E. Segal, Noise in gene expression is coupled to growth rate, Genome Res. 25, 1893 (2015), epub 2015-09-09

  2. [2]

    Quarton, T

    T. Quarton, T. Kang, V. Papakis, K. Nguyen, C. Nowak, Y. Li, and L. Bleris, Uncoupling gene expression noise along the central dogma using genome engineered human cell lines, Nucleic Acids Res.48, 9406 (2020)

  3. [3]

    J. D. Sipe and A. S. Cohen, Review: history of the amy- loid fibril, J. Struct. Biol.130, 88 (2000)

  4. [4]

    Eisenberg and M

    D. Eisenberg and M. Jucker, The amyloid state of pro- teins in human diseases, Cell148, 1188 (2012)

  5. [5]

    M. A. Gertz, A. Dispenzieri, and T. Sher, Pathophys- iology and treatment of cardiac amyloidosis, Nat. Rev. Cardiol.12, 91 (2015)

  6. [6]

    K. L. Moreau and J. A. King, Protein misfolding and aggregation in cataract disease and prospects for preven- tion, Trends Mol. Med.18, 273 (2012)

  7. [7]

    L. M. Dember, Amyloidosis-associated kidney disease, J. Am. Soc. Nephrol.17, 3458 (2006)

  8. [8]

    Schröder, Protein aggregate myopathies: the many faces of an expanding disease group, Acta Neuropathol

    R. Schröder, Protein aggregate myopathies: the many faces of an expanding disease group, Acta Neuropathol. 125, 1 (2013)

  9. [9]

    Chung, B

    C. Chung, B. M. Verheijen, Z. Navapanich,et al., Evolu- tionary conservation of the fidelity of transcription, Nat. Commun.14, 1547 (2023)

  10. [10]

    C. S. Chung, Y. Kou, S. J. Shemtov,et al., Transcript errors generate amyloid-like proteins in human cells, Nat. Commun.15, 8676 (2024)

  11. [11]

    X. Liu, D. A. Bushnell, and R. D. Kornberg, Rna polymerase ii transcription: structure and mechanism, Biochim. Biophys. Acta Gene Regul. Mech.1829, 2 (2013)

  12. [12]

    Vermulstet al., Transcription errors induce pro- teotoxic stress and shorten cellular lifespan, Nat

    M. Vermulstet al., Transcription errors induce pro- teotoxic stress and shorten cellular lifespan, Nat. Com- mun.6, 8065 (2015)

  13. [13]

    Peliti and S

    L. Peliti and S. Pigolotti,Stochastic thermodynamics: an introduction(Princeton University Press, 2021)

  14. [14]

    Mandal and C

    D. Mandal and C. Jarzynski, Work and information pro- cessing in a solvable model of maxwell’s demon, Proc. Natl. Acad. Sci. U.S.A.109, 11641 (2012)

  15. [15]

    Theory of Gases,

    J. C. Maxwell,Theory of Heat(Longmans, Green, and Co., London, 1871) see Chapter XXII, “Theory of Gases,” for Maxwell’s demon thought experiment

  16. [16]

    Szilard, On the decrease of entropy in a thermody- namic system by the intervention of intelligent beings, Z

    L. Szilard, On the decrease of entropy in a thermody- namic system by the intervention of intelligent beings, Z. Phys.65, 840 (1929)

  17. [17]

    Landauer, Irreversibility and heat generation in the computing process, IBM J

    R. Landauer, Irreversibility and heat generation in the computing process, IBM J. Res. Dev.5, 183 (1961)

  18. [18]

    C. H. Bennett, Demons, engines and the second law, Sci. Am.257, 108 (1987)

  19. [19]

    Deffner and C

    S. Deffner and C. Jarzynski, Information processing and the second law of thermodynamics: An inclusive, hamil- tonian approach, Phys. Rev. X3, 041003 (2013)

  20. [20]

    A. B. Boyd and J. P. Crutchfield, Identifying func- tional thermodynamics in autonomous maxwellian ratch- ets, New J. Phys.18, 023049 (2016)

  21. [21]

    A. B. Boyd, D. Mandal, and J. P. Crutchfield, 11 Correlation-powered information engines and the ther- modynamic efficiency of prediction, Phys. Rev. E95, 012152 (2017)

  22. [22]

    A.B.Boyd, D.Mandal,andJ.P.Crutchfield,Thermody- namics of temporal correlations, Phys. Rev. E97, 032129 (2018)

  23. [23]

    J. M. Horowitz and M. Esposito, Multipartite informa- tion flow for markov processes, J. Stat. Mech.: Theory Exp.2014(P03006)

  24. [24]

    Šafránek and S

    D. Šafránek and S. Deffner, Quantum zeno effect in cor- related qubits, Phys. Rev. A98, 032308 (2018)

  25. [25]

    A. B. Boyd, P. M. Riechers, and J. P. Crutchfield, Func- tional thermodynamics of maxwellian ratchets: Con- structing and deconstructing patterns, randomizing and derandomizing behaviors, Phys. Rev. Res.2, 033334 (2020)

  26. [26]

    A. B. Boyd and J. P. Crutchfield, Thermodynamics of prediction and adaptation in living systems, Theory Biosci.141, 167 (2022)

  27. [27]

    J. M. Horowitz and M. Esposito, Thermodynamics with continuous information flow, Phys. Rev. X4, 031015 (2014)

  28. [28]

    Sagawa and M

    T. Sagawa and M. Ueda, Fluctuation theorem with in- formation exchange: Role of correlations in stochastic thermodynamics, Phys. Rev. Lett.109, 180602 (2012)

  29. [29]

    Prokopenko and I

    M. Prokopenko and I. Einav, Information thermodynam- ics of near-equilibrium computation, Phys. Rev. E91, 062143 (2015)

  30. [30]

    Sone and S

    A. Sone and S. Deffner, Quantum and classical ergotropy from relative entropies, Entropy23, 10.3390/e23091107 (2021)

  31. [31]

    J. M. R. Parrondoet al., Information flows in nanoma- chines, arXiv (2023), arXiv:2312.02068 [cond-mat.stat- mech]

  32. [32]

    Stopnitzky, S.Still, T.E

    E. Stopnitzky, S.Still, T.E. Ouldridge,andL. Altenberg, Physical limitations of work extraction from temporal correlations, Phys. Rev. E99, 042115 (2019)

  33. [33]

    Cocconi and L

    L. Cocconi and L. Chen, Efficiency of an autonomous, dynamic information engine operating on a single active particle, Phys. Rev. E110, 014602 (2024)

  34. [34]

    S.S.ChittariandZ.Lu,Revisitingkineticmontecarloal- gorithms for time-dependent processes: From open-loop control to feedback control, J. Chem. Phys.161, 044104 (2024)

  35. [35]

    N. M. van Dijk, Uniformization for nonhomogeneous markov chains, Oper. Res. Lett.12, 241 (1992)

  36. [36]

    M. Arns, P. Buchholz, and A. Panchenko, On the numer- ical analysis of inhomogeneous continuous-time markov chains, INFORMS J. Comput.22, 416 (2010)

  37. [37]

    Y. Hsu, W. F. Wu, and J.-R. Chiou, Reliability anal- ysis based on nonhomogeneous continuous-time markov modelingwithapplicationtorepairablepumpsofapower plant, Int. J. Reliab. Qual. Saf. Eng.24, 1750004 (2017)

  38. [38]

    Lencastre, N

    P. Lencastre, N. Macedo, and P. G. Lind, From empiri- cal data to time-inhomogeneous continuous markov pro- cesses, Phys. Rev. E93, 032135 (2016)

  39. [39]

    Z. Ding, X. Guo, and H. Jiao, Markov chain approxima- tion and measure change for time-inhomogeneous diffu- sion processes, Appl. Math.Comput.387, 125024 (2021)

  40. [40]

    Truquet,Local Stationarity and Time-Inhomogeneous Markov Chains, Tech

    L. Truquet,Local Stationarity and Time-Inhomogeneous Markov Chains, Tech. Rep. (ENSAI, 2019) research re- port

  41. [41]

    Talkner, Statistics of entrance times, Physica A325, 124 (2003)

    P. Talkner, Statistics of entrance times, Physica A325, 124 (2003)

  42. [42]

    Talkner and J

    P. Talkner and J. Łuczka, Rate description of markov processes with time dependent parameters, Acta Phys. Pol. B36, 1837 (2005)

  43. [43]

    Forastiere, Linear stochastic thermodynamics, New J

    L. Forastiere, Linear stochastic thermodynamics, New J. Phys.24, 083021 (2022)

  44. [44]

    Rao and M

    R. Rao and M. Esposito, Detailed fluctuation theorems: A unifying perspective, Entropy20, 635 (2018)

  45. [45]

    Aslyamov and M

    T. Aslyamov and M. Esposito, Nonequilibrium response for markov jump processes: Exact results and tight bounds, Phys. Rev. Lett.132, 037101 (2024)

  46. [46]

    Á. M. Ledezma, Time-varying energy landscapes and temperature paths: Dynamic transition rates in lo- cally ultrametric complex systems, SSRN Electron. J. 10.2139/ssrn.5015668 (2024), arXiv:2411.03406 [cond- mat.stat-mech]

  47. [47]

    G. C. P. Innocentini, A. Hodgkinson, and O. Radulescu, Time dependent stochastic mrna and protein synthesis in piecewise-deterministic models of gene networks, Front. Phys.6, 46 (2018)

  48. [48]

    Jia and Y

    C. Jia and Y. Li, Analytical time-dependent distribu- tions for gene expression models with complex promoter switching mechanisms, SIAM J. Appl. Math.83, 1572 (2023)

  49. [49]

    B. Wu, J. Holehouse, R. Grima, and C. Jia, Solving the time-dependent protein distributions for autoregulated bursty gene expression using spectral decomposition, J. Chem. Phys.160, 074105 (2024)

  50. [50]

    Fintzi, X

    J. Fintzi, X. Cui, J. Wakefield, and V. N. Minin, Efficient data augmentation for fitting stochastic epidemic mod- els to prevalence data, J. Comput. Graph. Stat.26, 918 (2017)

  51. [51]

    S. L. Wu, J. B. Bennett, H. M. Sánchez C., A. J. Dolgert, T. M. León, and J. M. Marshall, Mgdrive 2: A simulation framework for gene drive systems incorporating season- ality and epidemiological dynamics, PLoS Comput. Biol. 17, e1009030 (2021)

  52. [52]

    R. Meng, B. Soper, H. K. Lee, J. F. Nygård, and M. Nygård, Hierarchical continuous-time inhomogeneous hidden markov model for cancer screening with extensive followup data, Stat. Methods Med. Res.31, 2383 (2022)

  53. [53]

    Qian, Open-system nonequilibrium steady state: Sta- tistical thermodynamics, fluctuations, and chemical os- cillations, J

    H. Qian, Open-system nonequilibrium steady state: Sta- tistical thermodynamics, fluctuations, and chemical os- cillations, J. Phys. Chem. B110, 15063 (2006)

  54. [54]

    M. L. Esquível, Statistics for continuous time markov chains, a short review, Axioms14, 283 (2025)

  55. [55]

    J. D. Watson and F. H. C. Crick, Molecular structure of nucleic acids: A structure for deoxyribose nucleic acid, Nature171, 737 (1953)

  56. [56]

    Grunberg-Manago and S

    M. Grunberg-Manago and S. Ochoa, Enzymatic synthe- sis of ribonucleic acid, Biochim. Biophys. Acta18, 495 (1955)

  57. [57]

    Kornberg, I

    A. Kornberg, I. R. Lehman, M. J. Bessman, and E. S. Simms, Enzymatic synthesis of deoxyribonucleic acid, J. Biol. Chem.219, 623 (1956)

  58. [58]

    Cramer, D

    P. Cramer, D. A. Bushnell, and R. D. Kornberg, Rna polymerase ii at 2.8 å resolution, Nature415, 253 (2001)

  59. [59]

    P. A. Levene and W. A. Jacobs, On the structure of yeast nucleic acid, J. Biol. Chem.7, 163 (1909)

  60. [60]

    Serreli, C

    V. Serreli, C. F. Lee, E. R. Kay, and D. A. Leigh, A molecular information ratchet, Nature445, 523 (2007)

  61. [61]

    R. E. Spinney, M. Prokopenko, and D. Chu, Informa- tion ratchets exploiting spatially structured information reservoirs, Phys. Rev. E98, 022124 (2018)

  62. [62]

    A. M. Jurgens and J. P. Crutchfield, Functional thermo- 12 dynamics of maxwellian ratchets: Constructing and de- constructing patterns, randomizing and derandomizing behaviors, Phys. Rev. Res.2, 033334 (2020)

  63. [63]

    P. D. Boyer, The atp synthase — a splendid molecular machine, Annu. Rev. Biochem.66, 717 (1997)

  64. [64]

    N. G. van Kampen,Stochastic Processes in Physics and Chemistry, 3rd ed. (Elsevier, 2007)

  65. [65]

    D. T. Gillespie, Exact stochastic simulation of coupled chemical reactions, J. Phys. Chem.81, 2340 (1977)

  66. [66]

    C. E. Shannon, A mathematical theory of communica- tion, Bell Syst. Tech. J.27, 379 (1948)

  67. [67]

    Nelson,Biological physics(W

    P. Nelson,Biological physics(W. H. Freeman, 2004)

  68. [68]

    R. Lipschitz, De explicatione per series trigonometricas instituenda functionum unius variabilis arbitrariarum, et praecipue earum, quae per variabilis spatium finitum val- orum maximourm et minimorum numerum habent infini- tum, disquisitio, J. Reine Angew. Math.63, 296 (1864)

  69. [69]

    Risken,The Fokker–Planck Equation: Methods of So- lution and Applications, 2nd ed., Springer Series in Syn- ergetics (Springer, Berlin, 1996)

    H. Risken,The Fokker–Planck Equation: Methods of So- lution and Applications, 2nd ed., Springer Series in Syn- ergetics (Springer, Berlin, 1996)

  70. [70]

    Chetrite and S

    R. Chetrite and S. Gupta, Two refreshing views of fluc- tuation theorems through kinematics elements and dy- namical symmetries, J. Stat. Phys.166, 1153 (2018)

  71. [71]

    Esposito and C

    M. Esposito and C. Van den Broeck, Three faces of the second law. i. master equation formulation, Phys. Rev. E 82, 011143 (2010)

  72. [72]

    F. Wang, Q. He, M. O’Donnell, and H. Li, Error- correcting processes maintain transcriptional fidelity in aging cells, bioRxiv , 2025.04.11.648458 (2025), preprint

  73. [73]

    D. T. Gillespie, Approximate accelerated stochastic sim- ulation of chemically reacting systems, J. Chem. Phys. 115, 1716 (2001)

  74. [74]

    Ander, P

    M. Ander, P. Beltrao, I. Ventura, R. Ferreira, and M. Rocha, Stochastic simulation of gene regulatory net- works, J. Theor. Biol.216, 367 (2002)

  75. [75]

    D. F. Anderson, A modified next reaction method for simulating chemical systems with time dependent propensities and delays, J. Chem. Phys.127, 214107 (2007)

  76. [76]

    Pillai, T

    S. Pillai, T. Suel, and S. Cha, The perron-frobenius theo- rem: some of its applications, IEEE Signal Process. Mag. 22, 62 (2005)

  77. [77]

    Edelman and B

    A. Edelman and B. D. Sutton, From random matrices to stochastic operators, J. Stat. Phys.127, 1121 (2007)