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Spectral Rigidity and Geometric Localization of Hopf Bifurcations in Planar Predator-Prey Systems

E. Chan-López, A. Martín-Ruiz, Víctor Castellanos

Abstract

We identify a geometric principle governing the location of Hopf and Bogdanov--Takens bifurcations in planar predator--prey systems. The prey coordinate of any coexistence equilibrium undergoing such a bifurcation lies between consecutive critical points of the prey nullcline. The mechanism is algebraic. At critical points of the nullcline, the vanishing of its derivative induces constraints on the Jacobian that prevent the spectral conditions required for bifurcation from being satisfied. We refer to this phenomenon as \emph{spectral rigidity}. The principle is established for three model families and one discrete counterpart with qualitatively different nullcline geometries: a quadratic case (Bazykin model), a cubic case (Holling type~IV with harvesting), and a rational case (Crowley--Martin functional response). In each case, the localization follows from explicit parametric characterizations and symbolic reduction. The analysis extends to discrete-time systems. For a map obtained by forward Euler discretization of the Crowley--Martin model, the Neimark--Sacker bifurcation occurs on the descending branch of the nullcline, providing a continuous--discrete duality governed by the same mechanism. We conjecture that this localization holds for general smooth prey nullclines, with critical points acting as spectral barriers that organise the bifurcation structure.

Spectral Rigidity and Geometric Localization of Hopf Bifurcations in Planar Predator-Prey Systems

Abstract

We identify a geometric principle governing the location of Hopf and Bogdanov--Takens bifurcations in planar predator--prey systems. The prey coordinate of any coexistence equilibrium undergoing such a bifurcation lies between consecutive critical points of the prey nullcline. The mechanism is algebraic. At critical points of the nullcline, the vanishing of its derivative induces constraints on the Jacobian that prevent the spectral conditions required for bifurcation from being satisfied. We refer to this phenomenon as \emph{spectral rigidity}. The principle is established for three model families and one discrete counterpart with qualitatively different nullcline geometries: a quadratic case (Bazykin model), a cubic case (Holling type~IV with harvesting), and a rational case (Crowley--Martin functional response). In each case, the localization follows from explicit parametric characterizations and symbolic reduction. The analysis extends to discrete-time systems. For a map obtained by forward Euler discretization of the Crowley--Martin model, the Neimark--Sacker bifurcation occurs on the descending branch of the nullcline, providing a continuous--discrete duality governed by the same mechanism. We conjecture that this localization holds for general smooth prey nullclines, with critical points acting as spectral barriers that organise the bifurcation structure.

Paper Structure

This paper contains 28 sections, 4 theorems, 28 equations, 1 figure.

Key Result

Theorem 3

Let $a$ be the bifurcation parameter in system eq:bazykin with $k > b > 0$. Then every coexistence equilibrium at which a Hopf bifurcation occurs satisfies

Figures (1)

  • Figure 1: Geometric localization of dynamic instabilities along the prey nullcline defined in \ref{['eq:cm_nullcline']}. The critical point $x_{\mathrm{v}}$ acts as a structural boundary induced by spectral rigidity. In the continuous--time formulation, the Hopf bifurcation is confined to the ascending branch (blue), whereas in discrete--time mappings, the Neimark--Sacker (N--S) bifurcation occurs on the descending branch (green). This geometric separation reflects the continuous--discrete duality of the underlying bifurcation mechanism.

Theorems & Definitions (18)

  • Definition 1
  • Example 2
  • Theorem 3: Quadratic Localization
  • proof : Proof sketch
  • Remark 4
  • Theorem 5: Cubic Localization
  • proof : Proof sketch
  • Theorem 6: Crowley--Martin Localization
  • proof
  • Remark 7: Recovery of the classical Hopf point
  • ...and 8 more