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arxiv: 2605.16753 · v1 · pith:IDCMOTKXnew · submitted 2026-05-16 · 🧬 q-bio.QM · math.DS

Viability Space Decomposition: A geometric partition of survival outcomes in single- and multi-agent systems

Pith reviewed 2026-05-19 19:50 UTC · model grok-4.3

classification 🧬 q-bio.QM math.DS
keywords viability space decompositionmortality manifoldsordering manifoldscollapse manifoldsviability portraitsurvival outcomesODE modelsmulti-agent systems
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The pith

Viability space decomposition partitions state space into regions of qualitatively similar survival outcomes using mortality, ordering, and collapse manifolds.

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

Models of living agents often use ordinary differential equations constrained to bounded viability regions, where leaving the region means death. Traditional tools like attractors and separatrices cannot fully describe the global space of behaviors because death is an absorbing outcome outside the viable set. The paper develops viability space decomposition to introduce mortality manifolds that bound viable regions, ordering manifolds that sequence distinct viability boundaries, and collapse manifolds that handle interactions in multi-agent cases. These elements together produce a viability portrait that classifies the entire state space by survival character. The approach is applied to three example models to show how it reveals complete global dynamics for subcellular networks, individual cells, and coupled cell systems.

Core claim

Viability space decomposition supplies a geometric partition of the state space for viability-constrained ODE models by identifying mortality manifolds that separate viable from non-viable states, ordering manifolds that rank successive viability limits, and collapse manifolds that resolve multi-agent interactions, thereby yielding a complete viability portrait of qualitatively distinct survival outcomes.

What carries the argument

Viability space decomposition, which uses mortality, ordering, and collapse manifolds to produce a viability portrait that partitions state space according to survival outcomes.

Load-bearing premise

The introduced manifolds can be identified and combined to achieve a complete decomposition of all survival outcomes for the full class of viability-constrained ODE models without leaving regions unclassified.

What would settle it

A viability-constrained ODE model in which some open regions of state space exhibit mixed or unclassified survival outcomes after all mortality, ordering, and collapse manifolds have been located.

Figures

Figures reproduced from arXiv: 2605.16753 by Connor McShaffrey, Randall D. Beer.

Figure 1
Figure 1. Figure 1: FIG. 1 [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3 [PITH_FULL_IMAGE:figures/full_fig_p008_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. In the network diagrams, normal arrows represent [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 [PITH_FULL_IMAGE:figures/full_fig_p015_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Combining all of the elements from Fig. 6 gives us [PITH_FULL_IMAGE:figures/full_fig_p016_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8 [PITH_FULL_IMAGE:figures/full_fig_p018_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: (b). This reveals the same peak values for the [PITH_FULL_IMAGE:figures/full_fig_p021_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: FIG. 10. The complete numerical exploration of the behaving cell model, comprising one million simulations per two-dimensional [PITH_FULL_IMAGE:figures/full_fig_p022_10.png] view at source ↗
read the original abstract

What determines whether an organism or collective will survive under particular conditions? This question is asked across the life sciences when determining adaptive fit, developing efficacious treatments for diseases, and assessing the risks posed by ecological shifts. To aid their investigations, researchers employ models of agents which must respect particular constraints to remain alive. By constraining the dynamics of these agents to bounded viability regions, these models form a class of extended dynamical systems where transient dynamics can lead to death, making traditional attractors and separatrices insufficient for characterizing the global space of possible behaviors. To remedy this, we develop viability space decomposition, an analysis framework for ordinary differential equation models of agents with viability constraints. We first introduce the general theory, revealing how several new classes of manifolds (mortality, ordering, and collapse) permit a complete decomposition of state space into regions of qualitatively similar survival outcomes: a viability portrait. We then demonstrate the method by completely analyzing the global behavior of three models: a subcellular network, a behaving cell with the same physiology, and two coupled cell networks. Finally, we finish by discussing how the framework scales and future directions for its development and application.

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 / 1 minor

Summary. The paper develops viability space decomposition, an analysis framework for ODE models of agents subject to viability constraints. It introduces mortality, ordering, and collapse manifolds that are claimed to enable a complete geometric partition of state space into regions of qualitatively similar survival outcomes (a viability portrait). The framework is demonstrated via full global analysis of three models: a subcellular network, a single behaving cell, and two coupled cells.

Significance. If the completeness claim holds, the work supplies a systematic geometric tool for characterizing global behavior in viability-constrained dynamical systems, where traditional attractors and separatrices are insufficient. The three explicit demonstrations provide concrete, reproducible examples of the method in action and could support falsifiable predictions about survival regions in biological models.

major comments (1)
  1. [General theory] General theory (prior to the demonstrations): the manuscript asserts that the new manifolds permit a complete decomposition for the full class of viability-constrained ODE models, yet no explicit theorem or proof is supplied that guarantees the manifolds can always be identified and that their union (together with viability regions) exhausts state space without unclassified trajectories or overlaps. The demonstrations are restricted to three low-dimensional cases with relatively simple viability boundaries; this leaves the generality claim load-bearing but unproven for higher-dimensional or topologically complex systems.
minor comments (1)
  1. [Abstract] The abstract refers to 'several new classes of manifolds' without giving their defining properties or construction; a brief definitional sentence would improve immediate readability.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their positive evaluation of the work's significance and for the constructive major comment. We address the concern regarding the general theory below.

read point-by-point responses
  1. Referee: [General theory] General theory (prior to the demonstrations): the manuscript asserts that the new manifolds permit a complete decomposition for the full class of viability-constrained ODE models, yet no explicit theorem or proof is supplied that guarantees the manifolds can always be identified and that their union (together with viability regions) exhausts state space without unclassified trajectories or overlaps. The demonstrations are restricted to three low-dimensional cases with relatively simple viability boundaries; this leaves the generality claim load-bearing but unproven for higher-dimensional or topologically complex systems.

    Authors: We agree that a formal theorem would strengthen the presentation of the general theory. In the revised manuscript we will add an explicit theorem stating that, under standard assumptions (Lipschitz continuity of the vector field and compactness of the viability region), the mortality, ordering, and collapse manifolds together with the viability regions form a partition of the state space with no unclassified trajectories or overlaps. The proof will proceed by showing that every initial condition has a unique forward orbit that either remains in the viability region for all time or intersects the viability boundary at a first time, after which the orbit is classified by the type of boundary intersection (mortality, ordering, or collapse). We will also include a brief discussion of the coordinate-free, dimension-independent nature of the construction, noting that while the three demonstrations are low-dimensional for computational clarity, the definitions and partition property extend directly to higher-dimensional and topologically more complex viability sets. We will add a remark on practical identification challenges in high dimensions without altering the theoretical completeness claim. revision: yes

Circularity Check

0 steps flagged

No significant circularity; framework introduces independent geometric constructs

full rationale

The paper defines viability space decomposition by introducing new manifold classes (mortality, ordering, collapse) as part of a general theory for viability-constrained ODEs, then applies them to three specific low-dimensional models. No step reduces a claimed prediction or completeness result to a fitted parameter, self-citation chain, or definitional renaming; the central decomposition is constructed explicitly from the stated geometric partitions rather than presupposing the target classification. Demonstrations remain illustrative rather than load-bearing for the general claim, and the derivation stays self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 1 invented entities

Abstract-only review limits visibility into specific free parameters or axioms; the core assumption is that viability-constrained ODEs require new manifold types beyond traditional attractors.

axioms (1)
  • domain assumption Models of agents with viability constraints form extended dynamical systems where transient dynamics can lead to death and traditional attractors/separatrices are insufficient.
    Directly stated in the abstract as the motivation and class of systems addressed.
invented entities (1)
  • mortality manifolds, ordering manifolds, collapse manifolds no independent evidence
    purpose: To enable complete decomposition of state space into regions of similar survival outcomes.
    New classes introduced by the framework as described in the abstract.

pith-pipeline@v0.9.0 · 5735 in / 1333 out tokens · 41908 ms · 2026-05-19T19:50:40.914193+00:00 · methodology

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Reference graph

Works this paper leans on

60 extracted references · 60 canonical work pages

  1. [1]

    This makes the set of molecules autocatalytic

    Model specification The single-cell physiology is composed of two molecu- lar species M = {M1, M2} which reciprocally catalyze each other and are synthesized from one of two food molecules F = {F1, F2} respectively. This makes the set of molecules autocatalytic. Fig. 4(a) depicts this cir- cuit with normal arrows representing material transfor- mation, ro...

  2. [2]

    Numerical exploration To approximate the possible existential outcomes in the single-cell physiology, we uniformly sample a million initial conditions in the range [Mi] ∈ [0, 20]. We then numerically integrate each initial condition for up to 800 arbitrary time units (ATU), and color the initial condi- tion according to whether it survives or violates one...

  3. [3]

    The complement of the viability region V α, colored black, corresponds to where the total survival time is zero because the agent cannot exist beyond its viability region

    This reveals five distinct regions. The complement of the viability region V α, colored black, corresponds to where the total survival time is zero because the agent cannot exist beyond its viability region. The viability boundary ∂Vα trivially separates this portion from the other subsets where the agent persists for at least some time. Within the viabil...

  4. [4]

    Viability portrait A phase portrait analysis within the cell’s viability region reveals two equilibrium points: a saddle node EPS = (4 .008, 2.407) (light green point) and a sta- ble equilibrium point EPΩ = (13 .811, 4.686) (dark blue point), shown in Fig. 5(b). Sampling the flow, we can see that the asymptotically viable trajectories (green) con- verge t...

  5. [5]

    gives an ordering manifold O shown as a purple con- tour that separates T ′ 1 and T ′ 2 (Fig. 5(c)). Zooming in closer around o and sampling another 160,000 initial con- ditions for improved resolution, we can clearly see that O separates the two regions while the W u branch belongs to T ′ 2 (Fig. 5(d)). This final manifold finishes carving out the differ...

  6. [6]

    Model specification Our behaving cell model has the same physiology and viability constraints as the previous model, with the main difference being that we now allow the cell to move in a one-dimensional environment, X, which has opposing gradients of food concentrations, established by the fol- lowing equations and illustrated in Fig. 4(c): [F1] = 10 0.2...

  7. [7]

    One representative slice is shown in Fig

    Numerical exploration As with the cell physiology in a fixed environment, we approximate the possible existential outcomes for the behaving cell by sampling a million initial con- ditions spanning [Mi] ∈ [0, 20] simulated for 200 ATU, except now for slices of the environment X = [−20, −15, −10, −5, 0, 5, 10, 15, 20]. One representative slice is shown in F...

  8. [8]

    Viability Portrait Similar to the protocell analysis without behavior, a phase portrait analysis within Vα reveals a stable equi- librium point EPΩ = (6 .434, 6.434, 0) (dark blue) and a saddle node EPS = (4.020, 4.020, 0) (light green) (Fig. 6(d)). The branches of the saddle node’s one-dimensional unstable manifold W u (red trajectories) either converge ...

  9. [9]

    Model specification Like the single-cell physiology model, our multi-agent model will be comprised of two cells, α = {α1, α2}, where [M1] and [M2] belong to each of these agents respectively (Fig. 4(b)). We assume that these molecules are synthe- sized from the same precursor food molecule, but beyond this the synthesis is the same as in Eqn. 38: S([Mi]) ...

  10. [10]

    Numerical exploration We sample a million initial conditions within the do- main of interaction of the two cells X and then simu- late their trajectories for 800 ATU, revealing six discon- nected regions of qualitatively distinct survival outcomes (Fig. 8(a)). Regions are given labels according to their sequence of asymptotically and transiently viable ou...

  11. [11]

    lift function

    Viability portrait Decomposing our two-cell state space demands that we understand how our agents’ dynamics unfold within the intersection of their viability regions X . A phase por- trait analysis of the unified state space reveals a stable equilibrium point EPX Ω = (7.167, 4.707) (dark blue point) and a saddle node EPX S = (2 .571, 8.716) (light green) ...

  12. [12]

    E. Schrödinger, What Is Life? The Physical Aspect of the Living Cell ; with Mind and Matter & Autobiographical Sketches, Canto Classics (Cambridge University Press, Cambridge ; New York, 1992)

  13. [13]

    Phillips, Schrödinger’s What Is Life? at 75, Cell Sys- tems 12, 465 (2021)

    R. Phillips, Schrödinger’s What Is Life? at 75, Cell Sys- tems 12, 465 (2021)

  14. [14]

    R. D. Beer and E. A. Di Paolo, The theoretical foun- dations of enaction: Precariousness, Biosystems 223, 104823 (2023)

  15. [15]

    Loreau, From Populations to Ecosystems: The- oretical Foundations for a New Ecological Synthesis , Monographs in Population Biology (Princeton University Press, Princeton, 2010)

    M. Loreau, From Populations to Ecosystems: The- oretical Foundations for a New Ecological Synthesis , Monographs in Population Biology (Princeton University Press, Princeton, 2010)

  16. [16]

    McShaffrey, E

    C. McShaffrey, E. Agmon, and R. D. Beer, Matters of life and death in computational cell biology, npj Syst Biol Appl 10.1038/s41540-026-00718-y (2026)

  17. [17]

    R. I. Joh and J. S. Weitz, To Lyse or Not to Lyse: Transient-Mediated Stochastic Fate Determination in Cells Infected by Bacteriophages, PLoS Comput Biol 7, e1002006 (2011). 23

  18. [18]

    Ghaffarizadeh, R

    A. Ghaffarizadeh, R. Heiland, S. H. Friedman, S. M. Mu- menthaler, and P. Macklin, PhysiCell: An open source physics-based cell simulator for 3-D multicellular sys- tems, PLoS Comput Biol 14, e1005991 (2018)

  19. [19]

    McShaffrey and R

    C. McShaffrey and R. Beer, Maintaining Viability with Multiple Needs, in 2022 IEEE Symposium Series on Computational Intelligence (SSCI) (IEEE, Singapore, Singapore, 2022) pp. 1523–1528

  20. [20]

    W. R. Ashby, The Physical Origin of Adaptation by Trial and Error, The Journal of General Psychology 32, 13 (1945)

  21. [21]

    W. R. Ashby, Design for a Brain , 2nd ed. (Springer Netherlands, Dordrecht, 1960)

  22. [22]

    R. D. Beer, A dynamical systems perspective on agent- environment interaction, Artificial Intelligence 72, 173 (1995)

  23. [23]

    Good Regulator Theorem

    N. Virgo, M. Biehl, M. Baltieri, and M. Capucci, A “Good Regulator Theorem” for Embodied Agents, in AL- IFE 2025: Ciphers of Life: Proceedings of the Artificial Life Conference 2025 (Kyoto, Japan, 2025) p. 46

  24. [24]

    E. O. Voit, A systems-theoretical framework for health and disease: Inflammation and preconditioning from an abstract modeling point of view, Mathematical Bio- sciences 217, 11 (2009)

  25. [25]

    J. D. Davis, C. M. Kumbale, Q. Zhang, and E. O. Voit, Dynamical systems approaches to personalized medicine, Current Opinion in Biotechnology 58, 168 (2019)

  26. [26]

    X. E. Barandiaran and M. D. Egbert, Norm-Establishing and Norm-Following in Autonomous Agency, Artificial Life 20, 5 (2014)

  27. [27]

    Aubin, A

    J.-P. Aubin, A. M. Bayen, and P. Saint-Pierre, Viabil- ity Theory: New Directions (Springer Berlin Heidelberg, Berlin, Heidelberg, 2011)

  28. [28]

    Himeoka, S

    Y. Himeoka, S. A. Horiguchi, and T. J. Kobayashi, The- oretical basis for cell deaths, Phys. Rev. Research 6, 043217 (2024)

  29. [29]

    M. D. Egbert and J. Pérez-Mercader, Methods for Mea- suring Viability and Evaluating Viability Indicators, Ar- tificial Life 24, 106 (2018)

  30. [30]

    Kolchinsky and D

    A. Kolchinsky and D. H. Wolpert, Semantic informa- tion, autonomous agency and non-equilibrium statistical physics, Interface Focus. 8, 20180041 (2018)

  31. [31]

    Bartlett, A

    S. Bartlett, A. W. Eckford, M. Egbert, M. Lingam, A. Kolchinsky, A. Frank, and G. Ghoshal, Physics of Life: Exploring Information as a Distinctive Feature of Living Systems, PRX Life 3, 037003 (2025)

  32. [32]

    Baltieri and K

    M. Baltieri and K. Suzuki, Mathematical approaches to the study of agents (2025)

  33. [33]

    H. J. Chiel and R. D. Beer, The brain has a body: Adap- tive behavior emerges from interactions of nervous sys- tem, body and environment, Trends in Neurosciences 20, 553 (1997)

  34. [34]

    Aihara and H

    K. Aihara and H. Suzuki, Theory of hybrid dynamical systems and its applications to biological and medical systems, Phil. Trans. R. Soc. A. 368, 4893 (2010)

  35. [35]

    M. G. Cortes, Y. Lin, L. Zeng, and G. Balázsi, From Bench to Keyboard and Back Again: A Brief History of Lambda Phage Modeling, Annu. Rev. Biophys. 50, 117 (2021)

  36. [36]

    Yuan and D

    J. Yuan and D. Ofengeim, A guide to cell death pathways, Nat Rev Mol Cell Biol 25, 379 (2024)

  37. [37]

    Abraham and C

    R. Abraham and C. D. Shaw, Dynamics–the Geometry of Behavior , 2nd ed., Studies in Nonlinearity, Vol. Part Three: Global Behavior (Addison-Wesley, Advanced Book Program, Redwood City, Calif, 1992)

  38. [38]

    F. J. Varela, Principles of Biological Autonomy , new annotated edition ed., edited by E. A. Di Paolo and E. Thompson (The MIT Press, Cambridge, Mas- sachusetts London, 2025)

  39. [39]

    H. R. Maturana, F. J. Varela, S. Beer, and H. R. Mat- urana, Autopoiesis and Cognition: The Realization of the Living , Boston Studies in the Philosophy of Sci- ence No. 42 (D. Reidel Publishing Company, Dordrecht Boston London, 1980)

  40. [40]

    R. D. Beer and P. L. Williams, Animals and Animats: Why Not Both Iguanas?, Adaptive Behavior 17, 296 (2009)

  41. [41]

    R. D. Beer, A.-S. Barwich, and G. J. Severino, Milking a spherical cow: Toy models in neuroscience, Eur J of Neuroscience 60, 6359 (2024)

  42. [42]

    S. A. Kauffman, Investigations (Oxford University Press- New York, NY, 2000)

  43. [43]

    Alon, An Introduction to Systems Biology: Design Principles of Biological Circuits , 2nd ed

    U. Alon, An Introduction to Systems Biology: Design Principles of Biological Circuits , 2nd ed. (Chapman and Hall/CRC, Second edition. | Boca Raton, Fla. : CRC Press, [2019], 2019)

  44. [44]

    McShaffrey and R

    C. McShaffrey and R. D. Beer, Decomposing Viability Space, in The 2023 Conference on Artificial Life (MIT Press, 2023)

  45. [45]

    Kalinin, S

    Y. Kalinin, S. Neumann, V. Sourjik, and M. Wu, Re- sponses of Escherichia coli Bacteria to Two Opposing Chemoattractant Gradients Depend on the Chemorecep- tor Ratio, J Bacteriol 192, 1796 (2010)

  46. [46]

    McShaffrey and R

    C. McShaffrey and R. D. Beer, Dissecting Viability in Multi-Agent Systems, in The 2024 Conference on Artifi- cial Life (MIT Press, Online, 2024)

  47. [47]

    J. R. Collier, N. A. Monk, P. K. Maini, and J. H. Lewis, Pattern Formation by Lateral Inhibition with Feedback: A Mathematical Model of Delta-Notch Intercellular Sig- nalling, Journal of Theoretical Biology 183, 429 (1996)

  48. [48]

    J. S. Lowengrub, H. B. Frieboes, F. Jin, Y.-L. Chuang, X. Li, P. Macklin, S. M. Wise, and V. Cristini, Nonlinear modelling of cancer: Bridging the gap between cells and tumours, Nonlinearity 23, R1 (2010)

  49. [49]

    J. E. Ferrell, Bistability, Bifurcations, and Waddington’s Epigenetic Landscape, Current Biology 22, R458 (2012)

  50. [50]

    Raju and E

    A. Raju and E. D. Siggia, A geometrical perspective on development, Dev Growth Differ 65, 245 (2023)

  51. [51]

    Goyal, G

    Y. Goyal, G. T. Busch, M. Pillai, J. Li, R. H. Boe, E. I. Grody, M. Chelvanambi, I. P. Dardani, B. Emert, N. Bodkin, J. Braun, D. Fingerman, A. Kaur, N. Jain, P. T. Ravindran, I. A. Mellis, K. Kiani, G. M. Alicea, M. E. Fane, S. S. Ahmed, H. Li, Y. Chen, C. Chai, J. Kaster, R. G. Witt, R. Lazcano, D. R. Ingram, S. B. Johnson, K. Wani, M. C. Dunagin, A. J....

  52. [52]

    Weiler, M

    P. Weiler, M. Lange, M. Klein, D. Pe’er, and F. Theis, CellRank 2: Unified fate mapping in multiview single-cell data, Nat Methods 21, 1196 (2024)

  53. [53]

    X. Qiu, Y. Zhang, J. D. Martin-Rufino, C. Weng, S. Hos- seinzadeh, D. Yang, A. N. Pogson, M. Y. Hein, K. Hoi (Joseph) Min, L. Wang, E. I. Grody, M. J. Shurtleff, R. Yuan, S. Xu, Y. Ma, J. M. Replogle, E. S. Lander, S. Darmanis, I. Bahar, V. G. Sankaran, J. Xing, and J. S. Weissman, Mapping transcriptomic vector fields of single cells, Cell 185, 690 (2022). 24

  54. [54]

    Pillai, E

    M. Pillai, E. Hojel, M. K. Jolly, and Y. Goyal, Unravel- ing non-genetic heterogeneity in cancer with dynamical models and computational tools, Nat Comput Sci 3, 301 (2023)

  55. [55]

    Islam and S

    S. Islam and S. Bhattacharya, Dynamical systems theory as an organizing principle for single-cell biology, npj Syst Biol Appl 11, 85 (2025)

  56. [56]

    Alon, Systems Medicine: Physiological Circuits and the Dynamics of Disease , 1st ed

    U. Alon, Systems Medicine: Physiological Circuits and the Dynamics of Disease , 1st ed. (Chapman and Hall/CRC, Boca Raton, 2023)

  57. [57]

    Forbes and C

    E. Forbes and C. McShaffrey, Analyzing minimum viable populations in deterministic community models using vi- ability space decomposition (2026)

  58. [58]

    Aguirre, R

    J. Aguirre, R. L. Viana, and M. A. F. Sanjuán, Fractal structures in nonlinear dynamics, Rev. Mod. Phys. 81, 333 (2009)

  59. [59]

    Krauskopf, H

    B. Krauskopf, H. M. Osinga, E. J. Doedel, M. E. Hender- son, J. Guckenheimer, A. Vladimirsky, M. Dellnitz, and O. Junge, A survey of methods for computing (un)stable manifolds of vector fields, Int. J. Bifurcation Chaos 15, 763 (2005)

  60. [60]

    McShaffrey and R

    C. McShaffrey and R. D. Beer, Shaking up viability space: Stochasticity and survival in the transient, in The 2025 Conference on Artificial Life (MIT Press, 2025)