Josef Hofbauer’s research while affiliated with University of Vienna and other places

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Publications (224)


A signaling game with payoff increments d1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$d_1$$\end{document} and d2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$d_2$$\end{document}, 0<d1<1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0< d_1 < 1$$\end{document}, 0<d2<1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0< d_2 < 1$$\end{document}, for the two types from using different signals. On top, the extensive form of the game in tree representation. Below, the normal-form representation—payoff matrix—of that extensive-form game
Nash equilibria and replicator dynamics as given by (9) of the game in Fig. 1 for the case 0<p<1/2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0
: The partially revealing equilibrium E1, which sits in the face (1,∗,∗,0)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(1,*,*,0)$$\end{document}, is surrounded by closed orbits, each of which attracts a three-dimensional manifold of nearby orbits. Arrows on the edges show the direction of the flow of the replicator dynamics. Edges without arrows consist of rest points
The two-dimensional face (1,∗,∗,0)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(1,*,*,0)$$\end{document} attracting all interior orbits of the replicator dynamics (9) and containing the partially revealing equilibrium E1 for the case 0<p<1/2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0
and three of its adjacent faces
Nash equilibria and replicator dynamics as given by (9) of the game in Fig. 1 for the case 1/2<p<1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$1/2
. Also shown is the connecting orbit from Ps¯s¯′=(0,0,1-d1,1)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$P'_{{{\bar{s}}} {{\bar{s}}}} = (0,0,1-d_1,1)$$\end{document} to (1,0,1,1) which reveals the instability of the component Ps¯s¯\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$P_{{{\bar{s}}} {{\bar{s}}}}$$\end{document}
The four two-dimensional faces that attract all interior orbits of the replicator dynamics (9) for 1/2<p<1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$1/2< p < 1$$\end{document}

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Evolutionary Dynamics of Signals with Type-specific Payoff Increments
  • Article
  • Full-text available

March 2025

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6 Reads

Dynamic Games and Applications

Josef Hofbauer

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Christina Pawlowitsch

This paper studies the replicator dynamics and the best-response dynamics of a signaling game with type-specific preferences over signals—a generalization of the beer-quiche game (Cho and Kreps in Q J Econ 102(2):179–221, 1987). When the prior probability of the high type is below the critical value at which player 2 is indifferent between accepting and not accepting, there is a unique, partially revealing equilibrium with partial pooling in the signal that the high type prefers. Under the replicator dynamics, this equilibrium is (Lyapunov) stable but not asymptotically stable. It is surrounded by periodic orbits each of which attracting a three-dimensional stable manifold from the interior of the state space. When the prior probability of the high type is above the critical value (the case usually considered), there are two equilibrium outcomes, each with pooling in one of the two signals. Under the replicator dynamics, the equilibrium outcome with pooling in the signal that the high type prefers is stable but not asymptotically stable. The equilibrium outcome with pooling in the signal that the low type prefers is unstable. Still, both components have basins of attraction with nonempty interior. The proofs use center manifold theory and chain recurrence. Throughout, results of the dynamic analysis are compared to equilibrium selection based on the intuitive criterion and index theory.

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The phase portrait of network 9 in Table 3 with 4κ1κ4<κ32\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$4\kappa _1\kappa _4<\kappa _3^2$$\end{document} and κ1=κ2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\kappa _1=\kappa _2$$\end{document} (left panel) and the bifurcation diagram with κ3,κ4>0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\kappa _3, \kappa _4>0$$\end{document} being fixed, while κ1,κ2>0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\kappa _1, \kappa _2>0$$\end{document} are parameters (right panel)
The 30 dynamically nonequivalent, bimolecular (2, 4, 2) mass-action networks that admit a fold bifurcation (see Theorem 25). The networks are partitioned into 3 groups. In each group, the first and the second reactions are the same for all networks (indicated in the top left corner), while the third and the fourth reactions are the row- and the column headers, respectively. A bullet indicates a fold bifurcation, while networks without a bullet do not admit a fold bifurcation. For the 10 networks marked with an orange bullet, the origin is an asymptotically stable equilibrium, and hence, these networks admit multiple attracting equilibria in the nonnegative quadrant. The 20 networks with a black bullet admit at most one asymptotically stable nonnegative equilibrium
The 198 dynamically nontrivial, quadratic, trimolecular (2, 4, 2) mass-action networks that admit an Andronov–Hopf bifurcation. The networks are partitioned into 7 groups. In each group, the first and the second reactions are the same for all networks (indicated in the top left corner), while the third and the fourth reactions are the row- and the column headers, respectively. In Group 7, the complex X+Y\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\textsf{X}+\textsf{Y}$$\end{document} is the reactant complex of two reactions, while it is the reactant complex of only one reaction for the networks in Groups 1–6. A green , a blue , or an orange symbol indicates that the Andronov–Hopf bifurcation is , , or , respectively. Notice that all three types of bifurcations occur for 3 networks in Group 2. The single network that admits a Bautin bifurcation is marked with the purple symbol ; the second focal value is positive. Networks without any symbol do not admit a positive equilibrium with a pair of purely imaginary eigenvalues
Bifurcations in planar, quadratic mass-action networks with few reactions and low molecularity

August 2024

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21 Reads

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4 Citations

Nonlinear Dynamics

In this paper we study bifurcations in mass-action networks with two chemical species and reactant complexes of molecularity no more than two. We refer to these as planar, quadratic networks as they give rise to (at most) quadratic differential equations on the nonnegative quadrant of the plane. Our aim is to study bifurcations in networks in this class with the fewest possible reactions, and the lowest possible product molecularity. We fully characterise generic bifurcations of positive equilibria in such networks with up to four reactions, and product molecularity no higher than three. In these networks we find fold, Andronov–Hopf, Bogdanov–Takens and Bautin bifurcations, and prove the non-occurrence of any other generic bifurcations of positive equilibria. In addition, we present a number of results which go beyond planar, quadratic networks. For example, we show that mass-action networks without conservation laws admit no bifurcations of codimension greater than m-2m2m-2, where m is the number of reactions; we fully characterise quadratic, rank-one mass-action networks admitting fold bifurcations; and we write down some necessary conditions for Andronov–Hopf and cusp bifurcations in mass-action networks. Finally, we draw connections with a number of previous results in the literature on nontrivial dynamics, bifurcations, and inheritance in mass-action networks.


Figure 1: The phase portrait of network 9 in Table 3 with 4κ 1 κ 4 < κ 2 3 and κ 1 = κ 2 (left panel) and the bifurcation diagram with κ 3 , κ 4 > 0 being fixed, while κ 1 , κ 2 > 0 are parameters (right panel).
Bifurcations in planar, quadratic mass-action networks with few reactions and low molecularity

June 2024

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20 Reads

In this paper we study bifurcations in mass-action networks with two chemical species and reactant complexes of molecularity no more than two. We refer to these as planar, quadratic networks as they give rise to (at most) quadratic differential equations on the nonnegative quadrant of the plane. Our aim is to study bifurcations in networks in this class with the fewest possible reactions, and the lowest possible product molecularity. We fully characterise generic bifurcations of positive equilibria in such networks with up to four reactions, and product molecularity no higher than three. In these networks we find fold, Andronov--Hopf, Bogdanov--Takens and Bautin bifurcations, and prove the non-occurrence of any other generic bifurcations of positive equilibria. In addition, we present a number of results which go beyond planar, quadratic networks. For example, we show that mass-action networks without conservation laws admit no bifurcations of codimension greater than m2m-2, where m is the number of reactions; we fully characterise quadratic, rank-one mass-action networks admitting fold bifurcations; and we write down some necessary conditions for Andronov--Hopf and cusp bifurcations in mass-action networks. Finally, we draw connections with a number of previous results in the literature on nontrivial dynamics, bifurcations, and inheritance in mass-action networks.


Oscillations in three‐reaction quadratic mass‐action systems

September 2023

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20 Reads

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8 Citations

Studies in Applied Mathematics

It is known that rank‐two bimolecular mass‐action systems do not admit limit cycles. With a view to understanding which small mass‐action systems admit oscillation, in this paper we study rank‐two networks with bimolecular source complexes but allow target complexes with higher molecularities. As our goal is to find oscillatory networks of minimal size, we focus on networks with three reactions, the minimum number that is required for oscillation. However, some of our intermediate results are valid in greater generality. One key finding is that an isolated periodic orbit cannot occur in a three‐reaction, trimolecular, mass‐action system with bimolecular sources. In fact, we characterize all networks in this class that admit a periodic orbit; in every case, all nearby orbits are periodic too. Apart from the well‐known Lotka and Ivanova reactions, we identify another network in this class that admits a center. This new network exhibits a vertical Andronov–Hopf bifurcation. Furthermore, we characterize all two‐species, three‐reaction, bimolecular‐sourced networks that admit an Andronov–Hopf bifurcation with mass‐action kinetics. These include two families of networks that admit a supercritical Andronov–Hopf bifurcation and hence a stable limit cycle. These networks necessarily have a target complex with a molecularity of at least four, and it turns out that there are exactly four such networks that are tetramolecular.


Stability and Fluctuations in Complex Ecological Systems

June 2023

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664 Reads

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Sarah Day

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[...]

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Els Weinans

From 08-12 August, 2022, 32 individuals participated in a workshop, Stability and Fluctuations in Complex Ecological Systems, at the Lorentz Center, located in Leiden, The Netherlands. An interdisciplinary dialogue between ecologists, mathematicians, and physicists provided a foundation of important problems to consider over the next 5-10 years. This paper outlines eight areas including (1) improving our understanding of the effect of scale, both temporal and spatial, for both deterministic and stochastic problems; (2) clarifying the different terminologies and definitions used in different scientific fields; (3) developing a comprehensive set of data analysis techniques arising from different fields but which can be used together to improve our understanding of existing data sets; (4) having theoreticians/computational scientists collaborate closely with empirical ecologists to determine what new data should be collected; (5) improving our knowledge of how to protect and/or restore ecosystems; (6) incorporating socio-economic effects into models of ecosystems; (7) improving our understanding of the role of deterministic and stochastic fluctuations; (8) studying the current state of biodiversity at the functional level, taxa level and genome level.


Oscillations in three-reaction quadratic mass-action systems

April 2023

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29 Reads

It is known that rank-two bimolecular mass-action systems do not admit limit cycles. With a view to understanding which small mass-action systems admit oscillation, in this paper we study rank-two networks with bimolecular source complexes but allow target complexes with higher molecularities. As our goal is to find oscillatory networks of minimal size, we focus on networks with three reactions, the minimum number that is required for oscillation. However, some of our intermediate results are valid in greater generality. One key finding is that an isolated periodic orbit cannot occur in a three-reaction, trimolecular, mass-action system with bimolecular sources. In fact, we characterise all networks in this class that admit a periodic orbit; in every case all nearby orbits are periodic too. Apart from the well-known Lotka and Ivanova reactions, we identify another network in this class that admits a center. This new network exhibits a vertical Andronov--Hopf bifurcation. Furthermore, we characterise all two-species, three-reaction, bimolecular-sourced networks that admit an Andronov--Hopf bifurcation with mass-action kinetics. These include two families of networks that admit a supercritical Andronov--Hopf bifurcation, and hence a stable limit cycle. These networks necessarily have a target complex with a molecularity of at least four, and it turns out that there are exactly four such networks that are tetramolecular.



Invasion graphs, -i\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$-i$$\end{document} communities, and sample simulations for two 5 species competitive Lotka-Volterra models. Vertex labels correspond to the species in the community. -i\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$-i$$\end{document} communities for which species i has a positive invasion growth rate are colored olive green, and otherwise gold. Lighter shaded vertices correspond to non-permanent communities, all others correspond to permanent communities. Thicker directed edges correspond to single species invasions. Green directed edges indicate transitions due to species i invading a -i\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$-i$$\end{document} community. Both models have acyclic invasion graphs, but only the model in the top panels allows for robust permanence. Sample simulations of the models are shown in the right hand panels. Parameter values in Appendix C
Periodic attractors for three competing species in a periodically-forced chemostat. In A, a periodic attractor at which all three species coexist (with a=0.3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$a=0.3$$\end{document}). In B, the mean densities of all three species along periodic attractors for increasing amplitude of the periodically-forced dilution rate. Parameter values: D0=0.4675\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$D_0=0.4675$$\end{document}, ω=0.2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\omega =0.2$$\end{document}, α1=1,α2=0.7,α3=0.64\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha _1=1,\alpha _2=0.7,\alpha _3=0.64$$\end{document}, β1=1,β2=0.3,β3=0.2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta _1=1,\beta _2=0.3,\beta _3=0.2$$\end{document}, R0=11\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ R _0=11$$\end{document}, and a=0.3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$a=0.3$$\end{document} in A and as shown in B
Invasion graphs for three competing species in a periodically-forced chemostat for increasing values of the amplitude a of the dilution rate. Shaded nodes correspond to -i\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$-i$$\end{document} subcommunities; olive green shading corresponds to a positive invasion growth rate of species i and yellow shading a negative invasion growth rate. Parameters as in Fig. 2
Permanence via invasion graphs: incorporating community assembly into modern coexistence theory

October 2022

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73 Reads

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27 Citations

Journal of Mathematical Biology

To understand the mechanisms underlying species coexistence, ecologists often study invasion growth rates of theoretical and data-driven models. These growth rates correspond to average per-capita growth rates of one species with respect to an ergodic measure supporting other species. In the ecological literature, coexistence often is equated with the invasion growth rates being positive. Intuitively, positive invasion growth rates ensure that species recover from being rare. To provide a mathematically rigorous framework for this approach, we prove theorems that answer two questions: (i) When do the signs of the invasion growth rates determine coexistence? (ii) When signs are sufficient, which invasion growth rates need to be positive? We focus on deterministic models and equate coexistence with permanence, i.e., a global attractor bounded away from extinction. For models satisfying certain technical assumptions, we introduce invasion graphs where vertices correspond to proper subsets of species (communities) supporting an ergodic measure and directed edges correspond to potential transitions between communities due to invasions by missing species. These directed edges are determined by the signs of invasion growth rates. When the invasion graph is acyclic (i.e. there is no sequence of invasions starting and ending at the same community), we show that permanence is determined by the signs of the invasion growth rates. In this case, permanence is characterized by the invasibility of all -ii-i communities, i.e., communities without species i where all other missing species have negative invasion growth rates. To illustrate the applicability of the results, we show that dissipative Lotka-Volterra models generically satisfy our technical assumptions and computing their invasion graphs reduces to solving systems of linear equations. We also apply our results to models of competing species with pulsed resources or sharing a predator that exhibits switching behavior. Open problems for both deterministic and stochastic models are discussed. Our results highlight the importance of using concepts about community assembly to study coexistence.


Figure 1. The phase portrait of ˙ p = −2κ 4 (e q − 1), ˙ q = κ 2 p. All nonconstant solutions are periodic.
The smallest bimolecular mass-action system with a vertical Andronov-Hopf bifurcation

October 2022

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22 Reads

We present a three-dimensional differential equation, which robustly displays a degenerate Andronov-Hopf bifurcation of infinite codimension, leading to a center, i.e., an invariant two-dimensional surface that is filled with periodic orbits surrounding an equilibrium. The system arises from a three-species bimolecular chemical reaction network consisting of four reactions. In fact, it is the only such mass-action system that admits a center via an Andronov-Hopf bifurcation.


Citations (74)


... In many cases, the above two networks are considered to be equivalent because when we only care about the dynamical behaviors determined by the steady states such as multistationarity, multistability, Hopf-bifurcation and ACR, we only need to study one of the networks that have the same steadystate ideal. Notice that relabeling the species or the reactions in a network naturally gives another kind of equivalence (see more details in [5] on the "dynamical equivalence" of networks). For instance, if we relabel the species X 1 and X 2 and we relabel the first and the second reactions in the network (1), then we get the following network ...

Reference:

An Efficient Algorithm for Determining the Equivalence of Zero-one Reaction Networks
Bifurcations in planar, quadratic mass-action networks with few reactions and low molecularity

Nonlinear Dynamics

... While there exist relevant general mathematical Chaos ARTICLE pubs.aip.org/aip/cha results about multistationarity, e.g., Balakotaiah and Luss (1982), Joshi and Shiu (2015), and Voitiuk and Pantea (2022), and oscillation, e.g., Póta (1983), Banaji and Boros (2023), and Banaji et al. (2024), no such work seems to exist about chaotic behavior; see Table I. Even in the recent special issue of Physica D, Katsanikas and Agaoglou (2021) titled "Chaos indicators, phase space and chemical reaction dynamics," there are no papers on chemical kinetics and the question of whether kinetic differential equations can show that chaotic behavior is not even mentioned. ...

Oscillations in three‐reaction quadratic mass‐action systems
  • Citing Article
  • September 2023

Studies in Applied Mathematics

... The equivalence of steady-state ideals is one of the equivalence problem in the field of chemical reaction networks. The dynamical features of chemical reaction networks such as multistability, Hopf-bifurcation, and absolute concentration robustness (ACR) are linked to switch-like behavior, decisionmaking process, oscillation, and so on in cellular signaling [7,23,27,9,3,25]. Usually, looking at the steady states is the first step for studying the dynamical behaviors of a chemical reaction system arising under mass-action kinetics. ...

The smallest bimolecular mass-action system with a vertical Andronov–Hopf bifurcation

Applied Mathematics Letters

... The copyright holder for this preprint this version posted February 15, 2025. ; https://doi.org/10.1101/2025.02.11.636978 doi: bioRxiv preprint invasibility framework of coexistence (Grainger et al., 2019;Hofbauer and Schreiber, 2022), along with non-traditional mechanisms of coexistence Levine et al., 2023;Zou et al., 2024;Godoy et al., 2024), or multiple alternative stable states in which species coexistence depends on the interplay between asymptotic and transient dynamics (Hofbauer and Schreiber, 2022;Spaak and Schreiber, 2023;Song1, 2024;Godoy et al., 2024). ...

Permanence via invasion graphs: incorporating community assembly into modern coexistence theory

Journal of Mathematical Biology

... Other than Andronov-Hopf and fold bifurcations of equilibria, nondegenerate Bogdanov-Takens bifurcations are also associated with homoclinic bifurcations [25,Section 6.2]. Examples of reaction systems displaying Bogdanov-Takens or homoclinic bifurcations appear in [4,13,17,21,23,24,26,27,29,30]. ...

Adding species to chemical reaction networks: Preserving rank preserves nondegenerate behaviours

Applied Mathematics and Computation

... Under assumptions of well-mixedness and a large number of reactants, systems arising from real-life applications can be modeled using the polynomial system described above. These include, in particular, chemical and biological interaction networks that exhibit diverse behaviors such as multistability [25,26], bifurcations [58,59], oscillations [10], homeostasis [18], and chaotic dynamics [35]. ...

Oscillations in Planar Deficiency-One Mass-Action Systems

Journal of Dynamics and Differential Equations

... wherex eq denotes the equilibrium concentrations, by constraining the intra-specific interactions, which are interactions within a single species, to be negative and to be diagonally dominant. 21,22 A realization of the complete model is randomly generated following the algorithm outlined in Appendix B. Realizations exhibit asymmetric competitive, cooperative, commensalistic, and predatory interactions. The intra-specific interactions are all competitive and are the dominant interaction of each species. ...

Diagonal dominance and harmless off-diagonal delays
  • Citing Article
  • February 2000

Proceedings of the American Mathematical Society

... Furthermore, toric dynamical systems are closely associated with the Global Attractor Conjecture, which proposes that such systems have a globally attracting steady state within each stoichiometric compatibility class. Various special cases of this conjecture have been proved [26,27,28,29]. An approach for a proof of this conjecture in full generality has been proposed in [18], using the idea of toric differential inclusions [30,20,31,32]. ...

Permanence of Weakly Reversible Mass-Action Systems with a Single Linkage Class
  • Citing Article
  • January 2020

SIAM Journal on Applied Dynamical Systems