México
México
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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