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Special Issue in Memory of Abdul-Aziz Yakubu

Adaptive delayed reproduction in a 2-dimensional discrete-time competition model

Article: 2248171 | Received 16 Mar 2023, Accepted 10 Aug 2023, Published online: 17 Aug 2023

Figures & data

Figure 1. The phase plane (x1,x2) of system (Equation1). The set D1 is a proper subset of D2. Species 1 is dominated by species 2. The unstable manifold of (X1,0) and the stable manifold of (0,X2) have nonempty intersections with the interior of R+2.

Figure 1. The phase plane (x1,x2) of system (Equation1(1) {x1(n+1)=x1(n){(1−η)exp⁡(λ−x1(n)−x2(n))+ηs}x2(n+1)=x2(n)exp⁡(λ−x1(n)−x2(n)),(1) ). The set D1 is a proper subset of D2. Species 1 is dominated by species 2. The unstable manifold of (X1,0) and the stable manifold of (0,X2) have nonempty intersections with the interior of R+2.

Table 1. Stability of the boundary fixed points and the boundary 2-cycles of system (Equation1).

Figure 2. The parameter plane (λ,s) of system (Equation1) with η0. In regions A, B, and C, (0,X2), P2, and P1 are asymptotically stable, respectively. There are no stable fixed points nor stable 2-cycles on the boundary of R+2 if λ>λ2.

Figure 2. The parameter plane (λ,s) of system (Equation1(1) {x1(n+1)=x1(n){(1−η)exp⁡(λ−x1(n)−x2(n))+ηs}x2(n+1)=x2(n)exp⁡(λ−x1(n)−x2(n)),(1) ) with η≈0. In regions A, B, and C, (0,X2), P2, and P1 are asymptotically stable, respectively. There are no stable fixed points nor stable 2-cycles on the boundary of R+2 if λ>λ2.

Figure 3. The parameter plane (λ,s) of system (Equation1). The green and red regions correspond to the region B and C in Figure , respectively. In the yellow region, both P1 and P2 have unstable transversal eigenvalues, i.e. both species can mutually invade at the boundary 2-cycles. On the left and right panels, η=0.01 and η=0.1, respectively.

Figure 3. The parameter plane (λ,s) of system (Equation1(1) {x1(n+1)=x1(n){(1−η)exp⁡(λ−x1(n)−x2(n))+ηs}x2(n+1)=x2(n)exp⁡(λ−x1(n)−x2(n)),(1) ). The green and red regions correspond to the region B and C in Figure 2, respectively. In the yellow region, both P1 and P2 have unstable transversal eigenvalues, i.e. both species can mutually invade at the boundary 2-cycles. On the left and right panels, η=0.01 and η=0.1, respectively.

Figure 4. The basins of attraction of the boundary 2-cycles of system (Equation1). The vertical and horizontal axes are x1 and x2, respectively. (a) The points in the green and yellow regions are attracted by (P1,0) and (P1,0), respectively, under the second iterate of system (Equation1). The parameters are λ=2.5, s = 0.6, and η=0.1. (b) The points in the black and red regions are attracted by (0,P2) and (0,P2), respectively, under the second iterate of system (Equation1). The parameters are λ=2.5, s = 0.1, and η=0.1.

Figure 4. The basins of attraction of the boundary 2-cycles of system (Equation1(1) {x1(n+1)=x1(n){(1−η)exp⁡(λ−x1(n)−x2(n))+ηs}x2(n+1)=x2(n)exp⁡(λ−x1(n)−x2(n)),(1) ). The vertical and horizontal axes are x1 and x2, respectively. (a) The points in the green and yellow regions are attracted by (P1,0) and (P1∗,0), respectively, under the second iterate of system (Equation1(1) {x1(n+1)=x1(n){(1−η)exp⁡(λ−x1(n)−x2(n))+ηs}x2(n+1)=x2(n)exp⁡(λ−x1(n)−x2(n)),(1) ). The parameters are λ=2.5, s = 0.6, and η=0.1. (b) The points in the black and red regions are attracted by (0,P2) and (0,P2∗), respectively, under the second iterate of system (Equation1(1) {x1(n+1)=x1(n){(1−η)exp⁡(λ−x1(n)−x2(n))+ηs}x2(n+1)=x2(n)exp⁡(λ−x1(n)−x2(n)),(1) ). The parameters are λ=2.5, s = 0.1, and η=0.1.

Figure 5. A single forward orbit of system (Equation1). The points of the orbit are connected with black and red lines if they are points of 2nth and 2n + 1th iteration, respectively. The parameters are the same as in Figure (a).

Figure 5. A single forward orbit of system (Equation1(1) {x1(n+1)=x1(n){(1−η)exp⁡(λ−x1(n)−x2(n))+ηs}x2(n+1)=x2(n)exp⁡(λ−x1(n)−x2(n)),(1) ). The points of the orbit are connected with black and red lines if they are points of 2nth and 2n + 1th iteration, respectively. The parameters are the same as in Figure 4 (a).