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Nullcline Geometry Constrains the Location of Oscillatory Instabilities in Planar Predator–Prey Systems

  • E. Chan-López [1] ; A. Martín-Ruiz [2] ; V. Castellanos [1]
    1. [1] Universidad Juárez Autónoma de Tabasco

      Universidad Juárez Autónoma de Tabasco

      México

    2. [2] Universidad Nacional Autónoma de México

      Universidad Nacional Autónoma de México

      México

  • Localización: Qualitative theory of dynamical systems, ISSN 1575-5460, Vol. 25, Nº 5, 2026
  • Idioma: inglés
  • Enlaces
  • Resumen
    • We prove that the critical structure of the prey nullcline constrains where oscillatory instabilities can emerge in planar predator–prey systems of Gause type. Under a predator self–damping hypothesis, the prey coordinate of every Hopf bifurcation point is confined to an ascending branch of the prey nullcline, between consecutive critical points. The mechanism is purely geometric: along the nullcline the diagonal Jacobian entry satisfies J11 = p(x) g (x), independently of the bifurcation parameter, while J22 < 0 at any coexistence equilibrium; at a critical point (g = 0) the trace is therefore strictly negative, so the critical points act as spectral barriers that preclude oscillatory onset. We illustrate the principle in three canonical families—Bazykin’s model (quadratic nullcline), a Leslie–Holling type IV system with harvesting (cubic nullcline), and the Crowley–Martin model with predator interference (rational nullcline)—for which we obtain closed–form Hopf loci. The mechanism persists in discrete time: for the forward Euler map with step size τ, the exact identity det(JG) − 1 = τ [tr(J ) + τ det(J )] shows that the Neimark–Sacker locus is strictly disjoint from the continuous Hopf locus, differs from it by the O(τ ) term τ det(J ), and crosses the spectral barrier only in the coarse–step regime. Predator saturation and interference thus not only bound the efficiency of interactions but also imprint a geometric architecture on the bifurcation landscape.

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